id stringlengths 9 14 | submitter stringlengths 1 56 ⌀ | authors stringlengths 5 835 | title stringlengths 5 209 | comments stringlengths 2 590 ⌀ | journal-ref stringlengths 11 239 ⌀ | doi stringlengths 14 94 ⌀ | report-no stringlengths 4 104 ⌀ | categories stringclasses 610
values | license stringclasses 9
values | orig_abstract stringlengths 22 2.01k | versions listlengths 1 16 | update_date stringdate 2007-05-23 00:00:00 2024-08-16 00:00:00 | authors_parsed listlengths 1 32 | abstract stringlengths 19 2.01k | perplexity_Llama-3.1-8B float64 2.29 655 | perplexity_s1-L-3.1-8B-base float64 2.77 362 | perplexity_s2-L-3.1-8B-base float64 3.14 496 | perplexity_s3-L-3.1-8B-base_v3 float64 2.9 431 | perplexity_s4-L-3.1-8B-base float64 2.88 422 | perplexity_s5-L-3.1-8B-base float64 2.95 414 | perplexity_s6-L-3.1-8B-base float64 2.99 340 | perplexity_s7-L-3.1-8B-base float64 2.91 467 | perplexity_s8-L-3.1-8B-base float64 2.89 220 | perplexity_s9-L-3.1-8B-base float64 3.21 1.68k | perplexity_s10-L-3.1-8B-base float64 2.98 600 | perplexity_s1-L-3.1-8B-qkv_v2 float64 2.92 729 | perplexity_s2-L-3.1-8B-qkv float64 3.05 621 | perplexity_s3-L-3.1-8B-qkv float64 2.96 631 | perplexity_s4-L-3.1-8B-qkv float64 2.86 570 | perplexity_s5-L-3.1-8B-qkv float64 2.93 558 | perplexity_s6-L-3.1-8B-qkv float64 2.96 669 | perplexity_s7-L-3.1-8B-qkv2 float64 2.95 682 | perplexity_s8-L-3.1-8B-qkv float64 2.92 502 | perplexity_s9-L-3.1-8B-qkv float64 3.06 549 | perplexity_s10-L-3.1-8B-qkv float64 2.95 795 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
hep-th/9407198 | null | Stefan Forste | A truly marginal deformation of SL(2,R) in a null direction | 6 pages, RI-8-94 (One reference and two footnotes added.) | Phys.Lett. B338 (1994) 36-39 | 10.1016/0370-2693(94)91340-4 | null | hep-th | null | We perform a marginal deformation of the SL(2,R) WZW model in a null
direction. If we send the deformation parameter to infinity we obtain a linear
dilaton background plus two free bosons. We show in addition that such a
background can be obtained by a duality transformation of the undeformed WZW
model. In the end we... | [
{
"created": "Sun, 31 Jul 1994 14:59:00 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Aug 1994 11:56:00 GMT",
"version": "v2"
}
] | 2009-10-28 | [
[
"Forste",
"Stefan",
""
]
] | We perform a marginal deformation of the SL(2,R) WZW model in a null direction. If we send the deformation parameter to infinity we obtain a linear dilaton background plus two free bosons. We show in addition that such a background can be obtained by a duality transformation of the undeformed WZW model. In the end we i... | 10.409324 | 8.826181 | 11.076159 | 8.438263 | 8.837354 | 8.982559 | 7.793716 | 8.039959 | 9.108606 | 11.634588 | 8.575738 | 8.366859 | 11.114863 | 9.478608 | 9.234004 | 8.992851 | 8.617303 | 8.915157 | 9.164823 | 10.561509 | 8.671399 |
1912.03181 | Matthew Yu | Ziqi Yan, Matthew Yu | Background Field Method for Nonlinear Sigma Models in Nonrelativistic
String Theory | 38 pages, 1 figure; v2: references added; v3: minor corrections | null | 10.1007/JHEP03(2020)181 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We continue the study of nonrelativistic string theory in background fields.
Nonrelativistic string theory is described by a nonlinear sigma model that maps
a relativistic worldsheet to a non-Lorentzian and non-Riemannian target space
geometry, which is known to be string Newton-Cartan geometry. We develop the
covari... | [
{
"created": "Fri, 6 Dec 2019 15:28:57 GMT",
"version": "v1"
},
{
"created": "Thu, 2 Apr 2020 16:55:13 GMT",
"version": "v2"
},
{
"created": "Tue, 9 Feb 2021 18:34:22 GMT",
"version": "v3"
}
] | 2021-02-10 | [
[
"Yan",
"Ziqi",
""
],
[
"Yu",
"Matthew",
""
]
] | We continue the study of nonrelativistic string theory in background fields. Nonrelativistic string theory is described by a nonlinear sigma model that maps a relativistic worldsheet to a non-Lorentzian and non-Riemannian target space geometry, which is known to be string Newton-Cartan geometry. We develop the covarian... | 5.463001 | 4.423128 | 5.903998 | 4.961976 | 4.91226 | 4.384578 | 4.486034 | 4.268991 | 4.766589 | 6.088325 | 4.800769 | 5.245676 | 5.431562 | 5.279363 | 4.928309 | 5.096614 | 5.040312 | 5.023435 | 5.05182 | 5.527479 | 4.986387 |
2011.13936 | Sebasti\'an C\'espedes | Sebastian Cespedes, Senarath P. de Alwis, Francesco Muia and Fernando
Quevedo | Lorentzian Vacuum Transitions: Open or Closed Universes? | 41 pages+ appendices, 15 figues. Minor rewording and references added | Phys. Rev. D 104, 026013 (2021) | 10.1103/PhysRevD.104.026013 | null | hep-th astro-ph.CO gr-qc | http://creativecommons.org/licenses/by/4.0/ | We consider the generalisation of quantum tunneling transitions in the WKB
approximation to the time-independent functional Schr\"odinger and
Wheeler-DeWitt equations. Following a Lorentzian approach, we compute the
transition rates among different scalar field vacua and compare with those
performed by Coleman and co... | [
{
"created": "Fri, 27 Nov 2020 19:00:01 GMT",
"version": "v1"
},
{
"created": "Thu, 10 Dec 2020 09:42:55 GMT",
"version": "v2"
}
] | 2021-08-04 | [
[
"Cespedes",
"Sebastian",
""
],
[
"de Alwis",
"Senarath P.",
""
],
[
"Muia",
"Francesco",
""
],
[
"Quevedo",
"Fernando",
""
]
] | We consider the generalisation of quantum tunneling transitions in the WKB approximation to the time-independent functional Schr\"odinger and Wheeler-DeWitt equations. Following a Lorentzian approach, we compute the transition rates among different scalar field vacua and compare with those performed by Coleman and coll... | 11.154801 | 12.198274 | 11.805922 | 11.537298 | 11.57827 | 11.9359 | 11.935208 | 11.196341 | 11.180161 | 12.660447 | 11.55226 | 11.373508 | 11.520097 | 11.307393 | 11.161641 | 11.374135 | 11.485076 | 11.22836 | 11.003547 | 11.390065 | 11.020153 |
hep-th/0211201 | David A. Lowe | Richard C. Brower, David A. Lowe and Chung-I Tan | Hagedorn transition for strings on pp-waves and tori with chemical
potentials | 15 pages, latex, references added and minor corrections | Nucl.Phys. B652 (2003) 127-141 | 10.1016/S0550-3213(03)00003-8 | BROWN-HET-1335 | hep-th | null | It has been conjectured that string theory in a pp-wave background is dual to
a sector of N=4 supersymmetric Yang-Mills theory.
We study the Hagedorn transition for free strings in this background. We find
that the free energy at the transition point is finite suggesting a
confinement/deconfinement transition in th... | [
{
"created": "Thu, 21 Nov 2002 19:21:37 GMT",
"version": "v1"
},
{
"created": "Mon, 2 Dec 2002 15:51:33 GMT",
"version": "v2"
}
] | 2010-04-05 | [
[
"Brower",
"Richard C.",
""
],
[
"Lowe",
"David A.",
""
],
[
"Tan",
"Chung-I",
""
]
] | It has been conjectured that string theory in a pp-wave background is dual to a sector of N=4 supersymmetric Yang-Mills theory. We study the Hagedorn transition for free strings in this background. We find that the free energy at the transition point is finite suggesting a confinement/deconfinement transition in the ga... | 7.671141 | 6.712238 | 8.941803 | 6.604668 | 6.755364 | 7.090084 | 6.816628 | 6.256578 | 6.090618 | 7.910502 | 6.698461 | 7.112524 | 7.530337 | 6.571107 | 7.018164 | 6.943831 | 7.009797 | 6.847051 | 6.675995 | 7.563646 | 6.728361 |
0912.2488 | Shin'ichi Nojiri | Shin'ichi Nojiri, Sergei D. Odintsov, Alexey Toporensky, and Petr
Tretyakov | Reconstruction and deceleration-acceleration transitions in modified
gravity | LaTeX 8 pages, published version. | Gen.Rel.Grav.42:1997-2008,2010 | 10.1007/s10714-010-0977-5 | null | hep-th astro-ph.CO gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the cosmological reconstruction in modified Gauss-Bonnet and F(R)
gravities. Two alternative representations of the action (with and without
auxiliary scalar) are considered. The approximate description of
deceleration-acceleration transition cosmologies is reconstructed. It is shown
that cosmological solu... | [
{
"created": "Sun, 13 Dec 2009 09:58:04 GMT",
"version": "v1"
},
{
"created": "Tue, 15 Dec 2009 23:12:11 GMT",
"version": "v2"
},
{
"created": "Thu, 25 Mar 2010 13:54:23 GMT",
"version": "v3"
}
] | 2014-11-20 | [
[
"Nojiri",
"Shin'ichi",
""
],
[
"Odintsov",
"Sergei D.",
""
],
[
"Toporensky",
"Alexey",
""
],
[
"Tretyakov",
"Petr",
""
]
] | We discuss the cosmological reconstruction in modified Gauss-Bonnet and F(R) gravities. Two alternative representations of the action (with and without auxiliary scalar) are considered. The approximate description of deceleration-acceleration transition cosmologies is reconstructed. It is shown that cosmological soluti... | 9.617702 | 9.47911 | 9.099694 | 8.80613 | 8.182979 | 9.652064 | 8.620313 | 8.528687 | 9.377258 | 9.478371 | 8.832366 | 8.85818 | 9.00474 | 8.907512 | 8.832664 | 8.910354 | 9.111339 | 8.936128 | 9.196717 | 8.969187 | 8.88569 |
0710.3564 | David A. Lowe | David A. Lowe | Some comments on embedding inflation in the AdS/CFT correspondence | 15 pages, 4 figures, revtex4 | Phys.Rev.D77:066003,2008 | 10.1103/PhysRevD.77.066003 | null | hep-th | null | The anti-de Sitter space/conformal field theory correspondence (AdS/CFT) can
potentially provide a complete formulation of string theory on a landscape of
stable and metastable vacua that naturally give rise to eternal inflation. As a
model for this process, we consider bubble solutions with de Sitter interiors,
obta... | [
{
"created": "Thu, 18 Oct 2007 17:52:41 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Lowe",
"David A.",
""
]
] | The anti-de Sitter space/conformal field theory correspondence (AdS/CFT) can potentially provide a complete formulation of string theory on a landscape of stable and metastable vacua that naturally give rise to eternal inflation. As a model for this process, we consider bubble solutions with de Sitter interiors, obtain... | 11.594809 | 13.060567 | 12.897316 | 10.814727 | 12.837221 | 12.11864 | 11.740657 | 11.620712 | 11.983929 | 13.417048 | 11.603269 | 11.732869 | 11.859812 | 11.407454 | 11.843112 | 11.581409 | 11.651259 | 11.544699 | 11.600289 | 11.900933 | 11.536836 |
hep-th/9503157 | Nekrassov Alexandrovich | Nikita Nekrasov | Holomorphic Bundles and Many-Body Systems | harvmac, 21 pages. In the revised version the formulas for the Lax
operator on the arbitrary genus curve are added | Commun.Math.Phys. 180 (1996) 587-604 | 10.1007/BF02099624 | PUPT-1534, ITEP-N95/1 | hep-th alg-geom math.AG | null | We show that spin generalization of elliptic Calogero-Moser system, elliptic
extension of Gaudin model and their cousins can be treated as a degenerations
of Hitchin systems. Applications to the constructions of integrals of motion,
angle-action variables and quantum systems are discussed. Explicit formulas for
the L... | [
{
"created": "Thu, 23 Mar 1995 20:09:43 GMT",
"version": "v1"
},
{
"created": "Fri, 24 Mar 1995 06:07:39 GMT",
"version": "v2"
},
{
"created": "Sun, 30 Apr 1995 23:28:36 GMT",
"version": "v3"
},
{
"created": "Mon, 1 May 1995 17:36:44 GMT",
"version": "v4"
}
] | 2009-10-28 | [
[
"Nekrasov",
"Nikita",
""
]
] | We show that spin generalization of elliptic Calogero-Moser system, elliptic extension of Gaudin model and their cousins can be treated as a degenerations of Hitchin systems. Applications to the constructions of integrals of motion, angle-action variables and quantum systems are discussed. Explicit formulas for the Lax... | 9.677825 | 9.891562 | 14.053639 | 9.122654 | 9.396567 | 9.558345 | 10.34049 | 9.366603 | 8.95145 | 12.803888 | 9.097791 | 9.162096 | 10.247444 | 9.017117 | 9.198522 | 8.96776 | 9.129432 | 9.283668 | 9.04077 | 10.361836 | 8.855752 |
2204.02981 | Atakan Hilmi F{\i}rat | Sergei Alexandrov, Atakan Hilmi F{\i}rat, Manki Kim, Ashoke Sen,
Bogdan Stefa\'nski jr | D-instanton Induced Superpotential | 34+31 pages; v2: references added | JHEP07(2022)090 | 10.1007/JHEP07(2022)090 | L2C:22-026, MIT-CTP/5416 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use string field theory to fix the normalization of the D-instanton
corrections to the superpotential involving the moduli fields of type II string
theory compactified on an orientifold of a Calabi-Yau threefold in the absence
of fluxes. We focus on $O(1)$ instantons whose only zero modes are the four
bosonic mode... | [
{
"created": "Wed, 6 Apr 2022 18:00:00 GMT",
"version": "v1"
},
{
"created": "Thu, 12 May 2022 13:49:30 GMT",
"version": "v2"
}
] | 2022-07-20 | [
[
"Alexandrov",
"Sergei",
""
],
[
"Fırat",
"Atakan Hilmi",
""
],
[
"Kim",
"Manki",
""
],
[
"Sen",
"Ashoke",
""
],
[
"Stefański",
"Bogdan",
"jr"
]
] | We use string field theory to fix the normalization of the D-instanton corrections to the superpotential involving the moduli fields of type II string theory compactified on an orientifold of a Calabi-Yau threefold in the absence of fluxes. We focus on $O(1)$ instantons whose only zero modes are the four bosonic modes ... | 7.093116 | 7.312975 | 7.470241 | 6.892612 | 7.492433 | 7.082345 | 7.37308 | 7.128075 | 6.491516 | 8.268913 | 6.945842 | 7.147527 | 7.067121 | 6.939057 | 6.91099 | 6.950703 | 7.1376 | 6.999032 | 7.018472 | 6.760436 | 6.977213 |
hep-th/9612163 | Billy D. Jones | Billy D. Jones and Robert J. Perry (The Ohio State University) | The Lamb Shift in a Light Front Hamiltonian Approach | 35 pages, latex, 5 postscript figures included | Phys.Rev. D55 (1997) 7715-7730 | 10.1103/PhysRevD.55.7715 | null | hep-th hep-ph nucl-th | null | Light-front Hamiltonian methods are being developed to attack bound-state
problems in QCD. In this paper we advance the state of the art for these
methods by computing the well-known Lamb shift in hydrogen starting from first
principles of QED. There are obvious but significant qualitative differences
between QED and... | [
{
"created": "Sun, 15 Dec 1996 23:03:55 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Jones",
"Billy D.",
"",
"The Ohio State University"
],
[
"Perry",
"Robert J.",
"",
"The Ohio State University"
]
] | Light-front Hamiltonian methods are being developed to attack bound-state problems in QCD. In this paper we advance the state of the art for these methods by computing the well-known Lamb shift in hydrogen starting from first principles of QED. There are obvious but significant qualitative differences between QED and Q... | 10.229112 | 9.268988 | 10.748005 | 9.917561 | 10.625015 | 9.691397 | 10.334141 | 9.774252 | 9.600581 | 11.236391 | 9.641393 | 9.661103 | 10.444406 | 10.241076 | 9.63594 | 9.762733 | 9.605666 | 9.890396 | 9.606823 | 10.010964 | 9.806854 |
hep-th/0612253 | Daniel Waldram | Jerome P. Gauntlett, Nakwoo Kim and Daniel Waldram | Supersymmetric AdS_3, AdS_2 and Bubble Solutions | v2: 33 pages, published version in JHEP | JHEP 0704:005,2007 | 10.1088/1126-6708/2007/04/005 | Imperial/TP/2006/JG/03 | hep-th | null | We present new supersymmetric AdS_3 solutions of type IIB supergravity and
AdS_2 solutions of D=11 supergravity. The former are dual to conformal field
theories in two dimensions with N=(0,2) supersymmetry while the latter are dual
to conformal quantum mechanics with two supercharges. Our construction also
includes A... | [
{
"created": "Fri, 22 Dec 2006 20:03:44 GMT",
"version": "v1"
},
{
"created": "Mon, 16 Jul 2007 14:54:30 GMT",
"version": "v2"
}
] | 2010-10-27 | [
[
"Gauntlett",
"Jerome P.",
""
],
[
"Kim",
"Nakwoo",
""
],
[
"Waldram",
"Daniel",
""
]
] | We present new supersymmetric AdS_3 solutions of type IIB supergravity and AdS_2 solutions of D=11 supergravity. The former are dual to conformal field theories in two dimensions with N=(0,2) supersymmetry while the latter are dual to conformal quantum mechanics with two supercharges. Our construction also includes AdS... | 4.837478 | 4.169762 | 5.619118 | 4.329025 | 4.674558 | 4.565002 | 4.277863 | 4.342783 | 4.596879 | 6.410899 | 4.329268 | 4.762932 | 5.253323 | 4.61097 | 4.527105 | 4.683623 | 4.598149 | 4.598897 | 4.627001 | 5.50224 | 4.546632 |
hep-th/0309042 | Gianmassimo Tasinato | H.-P. Nilles, A. Papazoglou, G. Tasinato (Bonn U.) | Selftuning and its footprints | 28 pages, JHEP style. v2: typos corrected and references added.
Published version | Nucl.Phys.B677:405-429,2004 | 10.1016/j.nuclphysb.2003.11.003 | null | hep-th astro-ph gr-qc hep-ph | null | We re-consider the self tuning idea in brane world models of finite volume.
We notice that in a large class of self tuning models, the four dimensional
physics is sensitive to the vacuum energy on the brane. In particular the
compactification volume changes each time the tension of the brane is modified:
consequently... | [
{
"created": "Wed, 3 Sep 2003 16:28:15 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Sep 2003 13:41:42 GMT",
"version": "v2"
},
{
"created": "Fri, 5 Dec 2003 09:03:54 GMT",
"version": "v3"
}
] | 2011-05-05 | [
[
"Nilles",
"H. -P.",
"",
"Bonn U."
],
[
"Papazoglou",
"A.",
"",
"Bonn U."
],
[
"Tasinato",
"G.",
"",
"Bonn U."
]
] | We re-consider the self tuning idea in brane world models of finite volume. We notice that in a large class of self tuning models, the four dimensional physics is sensitive to the vacuum energy on the brane. In particular the compactification volume changes each time the tension of the brane is modified: consequently, ... | 13.662837 | 11.959044 | 11.20557 | 10.696525 | 11.463984 | 11.517859 | 10.813618 | 11.164202 | 11.435925 | 11.83215 | 11.222183 | 11.427114 | 11.455478 | 11.066072 | 11.198243 | 11.617286 | 11.261801 | 11.026769 | 10.971263 | 11.519276 | 10.950786 |
hep-th/0212141 | Maria A. Lledo | L. Andrianopoli, R. D'Auria, S. Ferrara, M. A. Lledo | Gauged extended supergravity without cosmological constant: no-scale
structure and supersymmetry breaking | AMS-LaTeX, 16 pages. Invited paper to appear in the review section of
the IJMPA | Mod.Phys.Lett. A18 (2003) 1001-1012 | 10.1142/S0217732303009976 | CERN-TH/2002-346, UCLA/02/TEP/36 | hep-th | null | We consider the interplay of duality symmetries and gauged isometries of
supergravity models giving N-extended, spontaneously broken supergravity with a
no-scale structure. Some examples, motivated by superstring and M-theory
compactifications are described.
| [
{
"created": "Thu, 12 Dec 2002 15:03:29 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Andrianopoli",
"L.",
""
],
[
"D'Auria",
"R.",
""
],
[
"Ferrara",
"S.",
""
],
[
"Lledo",
"M. A.",
""
]
] | We consider the interplay of duality symmetries and gauged isometries of supergravity models giving N-extended, spontaneously broken supergravity with a no-scale structure. Some examples, motivated by superstring and M-theory compactifications are described. | 11.821938 | 9.267025 | 10.960737 | 9.899354 | 9.564108 | 9.67331 | 9.075084 | 9.813104 | 9.972374 | 14.299847 | 9.871091 | 10.125184 | 12.866856 | 10.394741 | 10.135116 | 10.674034 | 10.574583 | 10.229414 | 10.880373 | 12.118331 | 10.12339 |
hep-th/9404092 | Elias Kiritsis | E. Kiritsis and C. Kounnas (CERN) | Dynamical Topology Change in String Theory | LaTeX file, 17pp., CERN-TH.7219/94, LPTENS-94/11. (Discussions have
been clarified in several places) | Phys.Lett. B331 (1994) 51-62 | 10.1016/0370-2693(94)90942-3 | null | hep-th astro-ph gr-qc | null | Exact string solutions are presented, providing backgrounds where a dynamical
change of topology is occuring. This is induced by the time variation of a
modulus field. Some lessons are drawn concerning the region of validity of
effective theories and how they can be glued together, using stringy
information in the re... | [
{
"created": "Fri, 15 Apr 1994 13:05:28 GMT",
"version": "v1"
},
{
"created": "Sat, 23 Apr 1994 09:13:08 GMT",
"version": "v2"
},
{
"created": "Thu, 19 May 1994 19:27:17 GMT",
"version": "v3"
}
] | 2009-10-28 | [
[
"Kiritsis",
"E.",
"",
"CERN"
],
[
"Kounnas",
"C.",
"",
"CERN"
]
] | Exact string solutions are presented, providing backgrounds where a dynamical change of topology is occuring. This is induced by the time variation of a modulus field. Some lessons are drawn concerning the region of validity of effective theories and how they can be glued together, using stringy information in the regi... | 24.210747 | 18.229677 | 17.985468 | 17.301086 | 15.509448 | 16.01001 | 17.734161 | 15.413883 | 17.668026 | 17.54315 | 18.179565 | 19.852661 | 20.665089 | 19.770826 | 18.03183 | 18.402678 | 19.377047 | 18.561422 | 18.741005 | 20.752914 | 19.92037 |
hep-th/0701194 | Scott Chapman | Scott Chapman | Symmetry Breaking in BRST Quantization of SU(3) | null | null | null | null | hep-th | null | New BRST-invariant states for SU(3) gauge field theory are presented. The
states have finite norms and unlike the states that are usually used to derive
path integrals, they break SU(3) symmetry by choosing preferred gauge
directions. This symmetry breaking may also give effective masses to some of
the gauge bosons o... | [
{
"created": "Sun, 21 Jan 2007 22:43:22 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Chapman",
"Scott",
""
]
] | New BRST-invariant states for SU(3) gauge field theory are presented. The states have finite norms and unlike the states that are usually used to derive path integrals, they break SU(3) symmetry by choosing preferred gauge directions. This symmetry breaking may also give effective masses to some of the gauge bosons of ... | 16.721355 | 14.041186 | 14.457098 | 13.58609 | 14.809571 | 15.346397 | 16.070923 | 15.532742 | 15.073189 | 13.924121 | 15.291241 | 13.794659 | 14.099165 | 14.311954 | 13.995163 | 13.802551 | 13.862283 | 13.678909 | 14.039423 | 14.096147 | 14.438635 |
1005.5274 | Ram Brustein | Ram Brustein, A.J.M. Medved | Unitarity constraints on the ratio of shear viscosity to entropy density
in higher derivative gravity | Sign error in the equations of motion corrected, leading to several
numerical changes. Clarifications added, references added. Main results and
cnclusions essentially unchanged. V3 published version. Clarifications added,
discussion of Gauss-Bonnet moved to main text | Phys.Rev.D83:126005,2011 | 10.1103/PhysRevD.83.126005 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss corrections to the ratio of shear viscosity to entropy density
$\eta/s$ in higher-derivative gravity theories. Generically, these theories
contain ghost modes with Planck-scale masses. Motivated by general
considerations about unitarity, we propose new boundary conditions for the
equations of motion of the... | [
{
"created": "Fri, 28 May 2010 12:08:07 GMT",
"version": "v1"
},
{
"created": "Mon, 28 Jun 2010 07:25:08 GMT",
"version": "v2"
},
{
"created": "Mon, 25 Jul 2011 13:31:45 GMT",
"version": "v3"
}
] | 2011-07-26 | [
[
"Brustein",
"Ram",
""
],
[
"Medved",
"A. J. M.",
""
]
] | We discuss corrections to the ratio of shear viscosity to entropy density $\eta/s$ in higher-derivative gravity theories. Generically, these theories contain ghost modes with Planck-scale masses. Motivated by general considerations about unitarity, we propose new boundary conditions for the equations of motion of the g... | 5.387558 | 5.683869 | 5.370444 | 5.392167 | 5.542878 | 5.586375 | 5.432145 | 5.506337 | 5.337182 | 5.903087 | 5.503815 | 5.254011 | 5.588029 | 5.394016 | 5.30622 | 5.32013 | 5.393319 | 5.334336 | 5.31569 | 5.463219 | 5.317837 |
hep-th/9307102 | Palev Tchavpar | T. D. Palev and N. I. Stoilova | Wigner Quantum Oscillators | 8 pagex, TeX, IC/93/190 | J.Phys. A27 (1994) 977-984 | 10.1088/0305-4470/27/3/035 | null | hep-th | null | We present three groups of noncanonical quantum oscillators. The position and
the momentum operators of each of the groups generate basic Lie superalgebras,
namely $sl(1/3)$, $osp(1/6)$ and $osp(3/2)$. The $sl(1/3)$-oscillators have
finite energy spectrum and finite-dimensions. The $osp(1/6)$-oscillators are
related ... | [
{
"created": "Thu, 15 Jul 1993 16:01:00 GMT",
"version": "v1"
}
] | 2009-10-22 | [
[
"Palev",
"T. D.",
""
],
[
"Stoilova",
"N. I.",
""
]
] | We present three groups of noncanonical quantum oscillators. The position and the momentum operators of each of the groups generate basic Lie superalgebras, namely $sl(1/3)$, $osp(1/6)$ and $osp(3/2)$. The $sl(1/3)$-oscillators have finite energy spectrum and finite-dimensions. The $osp(1/6)$-oscillators are related to... | 6.916105 | 6.648839 | 7.034831 | 6.27953 | 6.904075 | 6.748218 | 6.787312 | 6.358129 | 7.081348 | 7.743048 | 6.456049 | 6.662195 | 6.909506 | 6.464175 | 6.420074 | 6.530709 | 6.68616 | 6.576368 | 6.404452 | 7.026483 | 6.534149 |
hep-th/0203014 | Massimo Porrati | M. Porrati | Fully Covariant Van Dam-Veltman-Zakharov Discontinuity, and Absence
Thereof | Inconsequential mistakes in Eqs. (12,13,20) corrected. 10 pages,
Latex. To appear in Physics Letters B | Phys.Lett.B534:209-215,2002 | 10.1016/S0370-2693(02)01656-8 | NYU-TH/02/02/01 | hep-th | null | In both old and recent literature, it has been argued that the celebrated van
Dam-Veltman-Zakharov (vDVZ) discontinuity of massive gravity is an artifact due
to linearization of the true equations of motion. In this letter, we
investigate that claim. First, we exhibit an explicit -albeit somewhat
arbitrary- fully cov... | [
{
"created": "Fri, 1 Mar 2002 18:06:09 GMT",
"version": "v1"
},
{
"created": "Fri, 12 Apr 2002 18:25:56 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Porrati",
"M.",
""
]
] | In both old and recent literature, it has been argued that the celebrated van Dam-Veltman-Zakharov (vDVZ) discontinuity of massive gravity is an artifact due to linearization of the true equations of motion. In this letter, we investigate that claim. First, we exhibit an explicit -albeit somewhat arbitrary- fully covar... | 6.374955 | 6.692342 | 6.475095 | 6.135303 | 6.725815 | 6.697359 | 6.314485 | 6.182268 | 6.288694 | 6.748578 | 6.345761 | 5.959399 | 6.239406 | 6.084673 | 6.227983 | 6.142545 | 6.145213 | 6.169185 | 6.097789 | 6.168777 | 6.063616 |
hep-th/9501112 | Filippo Colomo | Luca LUSANNA | Hamiltonian Constraints and Dirac's Observables: from Relativistic
Particles towards Field Theory and General Relativity. | Plain TEX, 15 pages, Talk given at the Workshop "Geometry of
Constrained Dynamical Systems", June 15-18, 1994, Cambridge, UK. | null | null | null | hep-th gr-qc | null | A review is given of the presymplectic approach to relativistic physical
systems and of the determination of their Dirac's observables. After
relativistic mechanics and Nambu string, the Dirac's observables of Yang-Mills
theory with fermions are given for the case of massless vector bosons (like in
QED). A Dirac-Yuka... | [
{
"created": "Tue, 24 Jan 1995 12:15:30 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"LUSANNA",
"Luca",
""
]
] | A review is given of the presymplectic approach to relativistic physical systems and of the determination of their Dirac's observables. After relativistic mechanics and Nambu string, the Dirac's observables of Yang-Mills theory with fermions are given for the case of massless vector bosons (like in QED). A Dirac-Yukawa... | 18.188044 | 18.448725 | 15.179139 | 15.915352 | 14.904921 | 18.023951 | 18.098108 | 15.827826 | 16.313503 | 18.078648 | 14.975574 | 15.990783 | 16.166716 | 16.202206 | 15.584693 | 16.271481 | 15.318995 | 15.4511 | 15.94514 | 16.006395 | 16.081709 |
hep-th/0002254 | Bervillier | C. Bagnuls and C. Bervillier | Renormalization group domains of the scalar Hamiltonian | 13 pages, 6 figures, to appear in Cond. Matt. Phys, some minor
corrections | Condensed Matter Phys.3:559,2000 | null | S00/013, T00/025 | hep-th cond-mat | null | Using the local potential approximation of the exact renormalization group
(RG) equation, we show the various domains of values of the parameters of the
O(1)-symmetric scalar Hamiltonian. In three dimensions, in addition to the
usual critical surface $S_{c}$ (attraction domain of the Wilson-Fisher fixed
point), we ex... | [
{
"created": "Tue, 29 Feb 2000 16:59:48 GMT",
"version": "v1"
},
{
"created": "Tue, 4 Apr 2000 12:45:41 GMT",
"version": "v2"
}
] | 2011-04-20 | [
[
"Bagnuls",
"C.",
""
],
[
"Bervillier",
"C.",
""
]
] | Using the local potential approximation of the exact renormalization group (RG) equation, we show the various domains of values of the parameters of the O(1)-symmetric scalar Hamiltonian. In three dimensions, in addition to the usual critical surface $S_{c}$ (attraction domain of the Wilson-Fisher fixed point), we expl... | 7.986856 | 8.543183 | 8.483301 | 7.882964 | 8.762855 | 8.497249 | 8.465034 | 8.216409 | 7.991235 | 9.181442 | 8.14627 | 7.91916 | 8.212225 | 7.843184 | 8.057703 | 7.841705 | 8.083001 | 7.733081 | 7.88478 | 8.161642 | 7.802508 |
hep-th/0406005 | Marcos Marino | Marcos Marino | Chern-Simons Theory and Topological Strings | 46 pages, RMP style, 25 figures, minor corrections, references added | Rev.Mod.Phys.77:675-720,2005 | 10.1103/RevModPhys.77.675 | CERN-PH-TH/2004-098 | hep-th | null | We review the relation between Chern-Simons gauge theory and topological
string theory on noncompact Calabi-Yau spaces. This relation has made possible
to give an exact solution of topological string theory on these spaces to all
orders in the string coupling constant. We focus on the construction of this
solution, w... | [
{
"created": "Tue, 1 Jun 2004 08:47:23 GMT",
"version": "v1"
},
{
"created": "Thu, 14 Oct 2004 12:34:12 GMT",
"version": "v2"
},
{
"created": "Fri, 6 May 2005 11:02:30 GMT",
"version": "v3"
},
{
"created": "Mon, 9 May 2005 09:55:51 GMT",
"version": "v4"
}
] | 2008-11-26 | [
[
"Marino",
"Marcos",
""
]
] | We review the relation between Chern-Simons gauge theory and topological string theory on noncompact Calabi-Yau spaces. This relation has made possible to give an exact solution of topological string theory on these spaces to all orders in the string coupling constant. We focus on the construction of this solution, whi... | 6.257802 | 5.970903 | 6.444477 | 5.305007 | 5.600354 | 5.380134 | 5.40907 | 5.201067 | 5.181279 | 7.434741 | 5.187758 | 5.603599 | 6.260045 | 5.593831 | 5.65528 | 5.566298 | 5.457915 | 5.602213 | 5.856421 | 6.136001 | 5.492194 |
1010.4946 | Pietro Menotti | Pietro Menotti | Riemann-Hilbert treatment of Liouville theory on the torus | 26 pages, LaTeX, references added, typos corrected | J.Phys.A44:115403,2011 | 10.1088/1751-8113/44/11/115403 | IFUP-TH/2010-38-r | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We apply a perturbative technique to study classical Liouville theory on the
torus. After mapping the problem on the cut-plane we give the perturbative
treatment for a weak source. When the torus reduces to the square the problem
is exactly soluble by means of a quadratic transformation in terms of
hypergeometric fun... | [
{
"created": "Sun, 24 Oct 2010 09:19:19 GMT",
"version": "v1"
},
{
"created": "Sun, 5 Dec 2010 14:57:21 GMT",
"version": "v2"
}
] | 2011-03-04 | [
[
"Menotti",
"Pietro",
""
]
] | We apply a perturbative technique to study classical Liouville theory on the torus. After mapping the problem on the cut-plane we give the perturbative treatment for a weak source. When the torus reduces to the square the problem is exactly soluble by means of a quadratic transformation in terms of hypergeometric funct... | 12.826962 | 12.847785 | 13.415005 | 12.188142 | 12.829021 | 12.918292 | 12.95146 | 12.425118 | 12.889587 | 13.792428 | 12.847752 | 12.499823 | 12.550789 | 12.567002 | 12.473512 | 12.868834 | 12.712459 | 12.333235 | 12.084684 | 12.572154 | 12.578882 |
hep-th/0610095 | Bernard Piette | B. Piette and W.J. Zakrzewski | Dynamical properties of a Soliton in a Potential Well | 21 pages, 27 figures | J.Phys.A40:329-346,2007 | 10.1088/1751-8113/40/2/011 | null | hep-th | null | We analyse the scattering of a two-dimensional soliton on a potential well.
We show that this soliton can pass through the well, bounce back or become
trapped and we study the dependence of the critical velocity on the width and
the depth of the well. We also present a model based on a pseudo-geodesic
approximation t... | [
{
"created": "Mon, 9 Oct 2006 13:46:46 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Piette",
"B.",
""
],
[
"Zakrzewski",
"W. J.",
""
]
] | We analyse the scattering of a two-dimensional soliton on a potential well. We show that this soliton can pass through the well, bounce back or become trapped and we study the dependence of the critical velocity on the width and the depth of the well. We also present a model based on a pseudo-geodesic approximation to ... | 7.568758 | 7.771061 | 7.367606 | 7.372909 | 7.702998 | 7.919842 | 7.383825 | 6.942782 | 7.004962 | 8.413401 | 6.794732 | 7.140819 | 7.26124 | 7.041698 | 7.310455 | 7.157294 | 7.162837 | 7.218876 | 7.128725 | 7.137855 | 7.056391 |
hep-th/9704145 | Pierre Vanhove | Michael B. Green (DAMTP), and Pierre Vanhove (Ecole Polytechnique) | D-instantons, Strings and M-theory | harvmac (b) 17 pages. v4: Some formulae corrected. Dimensions
corrected for eleven-dimensional expressions | Phys.Lett.B408:122-134,1997 | 10.1016/S0370-2693(97)00785-5 | DAMTP/97-31 -- CPTH-S501-0497 | hep-th | null | The R^4 terms in the effective action for M-theory compactified on a
two-torus are motivated by combining one-loop results in type II superstring
theories with the Sl(2,Z) duality symmetry. The conjectured expression
reproduces precisely the tree-level and one-loop R^4 terms in the effective
action of the type II str... | [
{
"created": "Mon, 21 Apr 1997 10:29:06 GMT",
"version": "v1"
},
{
"created": "Tue, 22 Apr 1997 18:44:57 GMT",
"version": "v2"
},
{
"created": "Thu, 19 Jun 1997 15:40:42 GMT",
"version": "v3"
},
{
"created": "Wed, 15 Dec 1999 15:52:04 GMT",
"version": "v4"
}
] | 2010-11-19 | [
[
"Green",
"Michael B.",
"",
"DAMTP"
],
[
"Vanhove",
"Pierre",
"",
"Ecole Polytechnique"
]
] | The R^4 terms in the effective action for M-theory compactified on a two-torus are motivated by combining one-loop results in type II superstring theories with the Sl(2,Z) duality symmetry. The conjectured expression reproduces precisely the tree-level and one-loop R^4 terms in the effective action of the type II strin... | 6.684179 | 6.153864 | 7.559422 | 6.089278 | 6.475008 | 6.463358 | 6.329246 | 6.341907 | 6.3177 | 8.318708 | 6.445604 | 6.251083 | 7.140929 | 6.468717 | 6.301188 | 6.301378 | 6.290489 | 6.429072 | 6.347988 | 7.088785 | 6.064753 |
hep-th/9607022 | Gabriela Grunfeld | C. G. Bollini and M. C. Rocca | Is the Higgs a visible particle ? | 8 pages, LaTex, no figures | Nuovo Cim. A110 (1997) 363-368 | 10.1007/BF03035887 | null | hep-th | null | We suggest that the Higgs might be unobservable as a free particle, due to
its origin at a symmetry breaking mechanism. The standard model is kept intact,
only the definition of the vacuum for the Higgs is changed. With the new
(natural) definition, the Higgs propagator is half advanced and half retarded.
This Green ... | [
{
"created": "Wed, 3 Jul 1996 16:02:26 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Bollini",
"C. G.",
""
],
[
"Rocca",
"M. C.",
""
]
] | We suggest that the Higgs might be unobservable as a free particle, due to its origin at a symmetry breaking mechanism. The standard model is kept intact, only the definition of the vacuum for the Higgs is changed. With the new (natural) definition, the Higgs propagator is half advanced and half retarded. This Green fu... | 16.741005 | 15.443564 | 15.729741 | 14.727192 | 16.287405 | 17.088062 | 16.890623 | 16.262482 | 14.683497 | 15.827682 | 16.033751 | 15.8579 | 16.669771 | 15.697566 | 15.76362 | 16.095631 | 15.518384 | 15.872967 | 15.991636 | 16.213068 | 16.367601 |
1707.05070 | Dine Ousmane Samary | Ezinvi Baloitcha, Vincent Lahoche, Dine Ousmane Samary | Energy momentum tensor for translation invariant renormalizable
noncommutative field theory | 12 pages | Eur. Phys. J. Plus (2018) 133: 515 | 10.1140/epjp/i2018-12339-8 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we derive the energy momentum tensor for the translation
invariant noncommutative Tanasa scalar field model. The Wilson regularization
procedure is used to improve this tensor and the local conservation property is
recovered. The same question is addressed in the case where the Moyal star
product is de... | [
{
"created": "Mon, 17 Jul 2017 10:05:44 GMT",
"version": "v1"
},
{
"created": "Tue, 20 Nov 2018 09:33:23 GMT",
"version": "v2"
}
] | 2018-12-21 | [
[
"Baloitcha",
"Ezinvi",
""
],
[
"Lahoche",
"Vincent",
""
],
[
"Samary",
"Dine Ousmane",
""
]
] | In this paper, we derive the energy momentum tensor for the translation invariant noncommutative Tanasa scalar field model. The Wilson regularization procedure is used to improve this tensor and the local conservation property is recovered. The same question is addressed in the case where the Moyal star product is defo... | 14.070477 | 14.323776 | 14.695103 | 13.346288 | 13.375282 | 14.353696 | 13.842945 | 13.749709 | 13.256016 | 16.077955 | 12.887428 | 12.748539 | 13.281068 | 12.996442 | 12.720827 | 13.122168 | 12.300791 | 12.690262 | 12.420886 | 12.904323 | 12.614585 |
hep-th/9607040 | Eduardo Marino | R.Banerjee and E.C.Marino | Explicit Bosonization of the Massive Thirring Model in 3+1 Dimensions | Latex, 7 pages | Phys.Rev. D56 (1997) 3763-3765 | 10.1103/PhysRevD.56.3763 | null | hep-th | null | We bosonize the Massive Thirring Model in 3+1D for small coupling constant
and arbitrary mass. The bosonized action is explicitly obtained both in terms
of a Kalb-Ramond tensor field as well as in terms of a dual vector field. An
exact bosonization formula for the current is derived. The small and large mass
limits o... | [
{
"created": "Thu, 4 Jul 1996 15:47:04 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Banerjee",
"R.",
""
],
[
"Marino",
"E. C.",
""
]
] | We bosonize the Massive Thirring Model in 3+1D for small coupling constant and arbitrary mass. The bosonized action is explicitly obtained both in terms of a Kalb-Ramond tensor field as well as in terms of a dual vector field. An exact bosonization formula for the current is derived. The small and large mass limits of ... | 8.455548 | 6.714948 | 7.38695 | 6.58132 | 7.198394 | 6.730604 | 6.600227 | 6.589908 | 6.53749 | 7.295497 | 6.637928 | 7.266239 | 7.231332 | 7.257274 | 7.147764 | 7.297871 | 7.171097 | 7.051861 | 6.810728 | 7.375326 | 7.181597 |
0809.4952 | Gregory Korchemsky | Z.Bajnok, J.Balog, B.Basso, G.P.Korchemsky and L.Palla | Scaling function in AdS/CFT from the O(6) sigma model | 25 pages, 2 figures | Nucl.Phys.B811:438-462,2009 | 10.1016/j.nuclphysb.2008.11.023 | LPT-Orsay-08-76, ITP-Budapest Report No. 642 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Asymptotic behavior of the anomalous dimensions of Wilson operators with high
spin and twist is governed in planar N=4 SYM theory by the scaling function
which coincides at strong coupling with the energy density of a two-dimensional
bosonic O(6) sigma model. We calculate this function by combining the two-loop
corre... | [
{
"created": "Mon, 29 Sep 2008 12:24:26 GMT",
"version": "v1"
}
] | 2009-02-02 | [
[
"Bajnok",
"Z.",
""
],
[
"Balog",
"J.",
""
],
[
"Basso",
"B.",
""
],
[
"Korchemsky",
"G. P.",
""
],
[
"Palla",
"L.",
""
]
] | Asymptotic behavior of the anomalous dimensions of Wilson operators with high spin and twist is governed in planar N=4 SYM theory by the scaling function which coincides at strong coupling with the energy density of a two-dimensional bosonic O(6) sigma model. We calculate this function by combining the two-loop correct... | 7.776378 | 6.678688 | 8.113751 | 6.161553 | 6.946194 | 6.46027 | 6.849659 | 6.727156 | 6.704735 | 10.863853 | 6.732542 | 6.959055 | 7.672657 | 7.103071 | 6.858068 | 6.951982 | 6.93908 | 7.186393 | 6.861338 | 7.876297 | 7.042754 |
1912.06261 | Kei-Ichi Kondo | Kei-Ichi Kondo, Yui Hayashi, Ryutaro Matsudo, Yutaro Suda and Masaki
Watanabe | Complex poles, spectral function and reflection positivity violation of
Yang-Mills theory | 1+6 pages, plenary talk presented at Light Cone 2019 - QCD on the
light cone: from hadrons to heavy ions, 16-20 September 2019 held at Ecole
Polytechnique, Palaiseau, France | null | null | CHIBA-EP-243 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We discuss the analytic continuation of the gluon propagator from the
Euclidean region to the complex squared-momentum plane towards the Minkowski
region from a viewpoint of gluon confinement. For this purpose, we investigate
the massive Yang-Mills model with one-loop quantum corrections, which is to be
identified wi... | [
{
"created": "Thu, 12 Dec 2019 23:15:28 GMT",
"version": "v1"
}
] | 2019-12-16 | [
[
"Kondo",
"Kei-Ichi",
""
],
[
"Hayashi",
"Yui",
""
],
[
"Matsudo",
"Ryutaro",
""
],
[
"Suda",
"Yutaro",
""
],
[
"Watanabe",
"Masaki",
""
]
] | We discuss the analytic continuation of the gluon propagator from the Euclidean region to the complex squared-momentum plane towards the Minkowski region from a viewpoint of gluon confinement. For this purpose, we investigate the massive Yang-Mills model with one-loop quantum corrections, which is to be identified with... | 5.69424 | 5.452534 | 6.006563 | 5.390914 | 5.557208 | 5.529646 | 5.60791 | 5.266643 | 5.252401 | 6.921809 | 5.494771 | 5.558938 | 5.91683 | 5.706933 | 5.671793 | 5.782561 | 5.649807 | 5.590375 | 5.512825 | 5.790991 | 5.55781 |
1510.03407 | Akane Oikawa | Hiroyuki Abe, Akane Oikawa, and Hajime Otsuka | Wavefunctions on magnetized branes in the conifold | 38 pages, 2 figures | null | 10.1007/JHEP07(2016)054 | WU-HEP-15-12 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study wavefunctions on D$7$-branes with magnetic fluxes in the conifold.
Since some supersymmetric embeddings of D-branes on the $AdS_5\times T^{1,1}$
geometry are known, we consider one of the embeddings, especially the spacetime
filling D$7$-branes in which (a part of) the standard model is expected to be
realiz... | [
{
"created": "Mon, 12 Oct 2015 19:40:11 GMT",
"version": "v1"
}
] | 2016-08-03 | [
[
"Abe",
"Hiroyuki",
""
],
[
"Oikawa",
"Akane",
""
],
[
"Otsuka",
"Hajime",
""
]
] | We study wavefunctions on D$7$-branes with magnetic fluxes in the conifold. Since some supersymmetric embeddings of D-branes on the $AdS_5\times T^{1,1}$ geometry are known, we consider one of the embeddings, especially the spacetime filling D$7$-branes in which (a part of) the standard model is expected to be realized... | 7.355629 | 6.767707 | 6.427932 | 6.375758 | 6.827124 | 6.805625 | 6.975572 | 6.869952 | 6.218123 | 6.934552 | 6.584941 | 6.696709 | 6.667152 | 6.480251 | 6.65664 | 6.751781 | 6.574247 | 6.979978 | 6.650643 | 6.701711 | 6.598146 |
hep-th/0104196 | A. Kapustnikov | A. Kapustnikov and A. Shcherbakov | Linear and nonlinear realizations of superbranes | 8 pages, LaTeX + espcrc2.sty The talk given at the D. Volkov Memorial
Conference SQFT, July, 25-29, 2000 | Nucl.Phys.Proc.Suppl. 102 (2001) 42-49 | 10.1016/S0920-5632(01)01534-1 | null | hep-th | null | The coordinate transformations which establish the direct relationship
between the actions of linear and nonlinear realizations of supermembranes are
proposed. It is shown that the Rocek-Tseytlin constraint known in the framework
of the linear realization of the theory is simply equivalent to a limit of a
"pure" nonl... | [
{
"created": "Mon, 23 Apr 2001 16:21:57 GMT",
"version": "v1"
},
{
"created": "Tue, 24 Apr 2001 15:55:17 GMT",
"version": "v2"
}
] | 2009-11-07 | [
[
"Kapustnikov",
"A.",
""
],
[
"Shcherbakov",
"A.",
""
]
] | The coordinate transformations which establish the direct relationship between the actions of linear and nonlinear realizations of supermembranes are proposed. It is shown that the Rocek-Tseytlin constraint known in the framework of the linear realization of the theory is simply equivalent to a limit of a "pure" nonlin... | 19.181643 | 18.856703 | 22.073114 | 17.265125 | 17.911337 | 17.71607 | 18.304041 | 15.75615 | 18.033726 | 20.458565 | 18.52252 | 17.03063 | 17.163378 | 15.968232 | 17.491388 | 16.299631 | 16.93317 | 15.83791 | 17.586771 | 17.515955 | 15.545219 |
1312.3871 | Peter Millington | Robert Dickinson, Jeff Forshaw, Peter Millington and Brian Cox | Manifest causality in quantum field theory with sources and detectors | 24 pages; 6 figures; version accepted for publication in JHEP | JHEP06(2014)049 | 10.1007/JHEP06(2014)049 | MAN/HEP/2013/25, IPPP/13/101, DCPT/13/202 | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We introduce a way to compute scattering amplitudes in quantum field theory
including the effects of particle production and detection. Our amplitudes are
manifestly causal, by which we mean that the source and detector are always
linked by a connected chain of retarded propagators. We show how these
amplitudes can b... | [
{
"created": "Fri, 13 Dec 2013 16:50:58 GMT",
"version": "v1"
},
{
"created": "Fri, 14 Feb 2014 15:02:09 GMT",
"version": "v2"
},
{
"created": "Mon, 16 Jun 2014 16:30:25 GMT",
"version": "v3"
}
] | 2014-06-17 | [
[
"Dickinson",
"Robert",
""
],
[
"Forshaw",
"Jeff",
""
],
[
"Millington",
"Peter",
""
],
[
"Cox",
"Brian",
""
]
] | We introduce a way to compute scattering amplitudes in quantum field theory including the effects of particle production and detection. Our amplitudes are manifestly causal, by which we mean that the source and detector are always linked by a connected chain of retarded propagators. We show how these amplitudes can be ... | 7.46468 | 6.965318 | 7.502875 | 6.415181 | 7.301812 | 6.775408 | 7.232454 | 6.581641 | 6.225388 | 7.643601 | 6.89017 | 6.886469 | 7.108768 | 6.854271 | 6.962831 | 7.185105 | 6.951047 | 6.949814 | 6.725014 | 7.118357 | 6.829903 |
hep-th/0407248 | Eugen Radu | Eugen Radu and Elizabeth Winstanley | Static axially symmetric solutions of Einstein-Yang-Mills equations with
a negative cosmological constant: black hole solutions | 47 pages, 47 figures | Phys.Rev. D70 (2004) 084023 | 10.1103/PhysRevD.70.084023 | null | hep-th gr-qc | null | We investigate static axially symmetric black hole solutions in a
four-dimensional Einstein-Yang-Mills-SU(2) theory with a negative cosmological
constant $\Lambda$. These solutions approach asymptotically the anti-de Sitter
spacetime and possess a regular event horizon. A discussion of the main
properties of the solu... | [
{
"created": "Wed, 28 Jul 2004 16:29:13 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Sep 2004 08:02:41 GMT",
"version": "v2"
}
] | 2009-11-10 | [
[
"Radu",
"Eugen",
""
],
[
"Winstanley",
"Elizabeth",
""
]
] | We investigate static axially symmetric black hole solutions in a four-dimensional Einstein-Yang-Mills-SU(2) theory with a negative cosmological constant $\Lambda$. These solutions approach asymptotically the anti-de Sitter spacetime and possess a regular event horizon. A discussion of the main properties of the soluti... | 5.673644 | 5.347659 | 5.136328 | 4.998431 | 5.519564 | 5.2399 | 5.007162 | 4.8302 | 5.37846 | 5.593097 | 5.439548 | 5.538605 | 5.375032 | 5.46488 | 5.482957 | 5.701673 | 5.450317 | 5.488879 | 5.491891 | 5.667932 | 5.531141 |
hep-th/0003083 | Hugo Compean | H. Garcia-Compean, O. Obregon and C. Ramirez | Searching for S-duality in Gravitation | 8+1 pages, LaTeX file, no figures. Invited talk at the `Third
Workshop on Gravitation and Mathematical Physics', Leon Gto. Mexico | null | null | CINVESTAV-FIS 12/00 | hep-th | null | We overview some attempts to find S-duality analogues of non-supersymmetric
Yang-Mills theory, in the context of gravity theories. The case of
MacDowell-Mansouri gauge theory of gravity is discussed. Three-dimensional
dimensional reductions from the topological gravitational sector in four
dimensions, enable to recup... | [
{
"created": "Fri, 10 Mar 2000 21:07:39 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Garcia-Compean",
"H.",
""
],
[
"Obregon",
"O.",
""
],
[
"Ramirez",
"C.",
""
]
] | We overview some attempts to find S-duality analogues of non-supersymmetric Yang-Mills theory, in the context of gravity theories. The case of MacDowell-Mansouri gauge theory of gravity is discussed. Three-dimensional dimensional reductions from the topological gravitational sector in four dimensions, enable to recuper... | 14.780312 | 12.805475 | 14.325388 | 12.735244 | 14.120287 | 13.224518 | 12.671859 | 12.384378 | 12.170972 | 14.044686 | 13.141557 | 12.887575 | 13.488686 | 13.283775 | 13.46302 | 13.727472 | 13.501423 | 13.299344 | 13.422411 | 13.235599 | 13.335709 |
hep-th/0001085 | Theodore A. Jacobson | Ted Jacobson | Trans-Planckian redshifts and the substance of the space-time river | 18 pages, to appear in Progress of Theoretical Physics Supplement,
Proceedings of Yukawa International Seminar 1999; typos corrected | Prog.Theor.Phys.Suppl.136:1-17,1999 | 10.1143/PTPS.136.1 | null | hep-th cond-mat gr-qc | null | Trans-Planckian redshifts in cosmology and outside black holes may provide
windows on a hypothetical short distance cutoff on the fundamental degrees of
freedom. In cosmology, such a cutoff seems to require a growing Hilbert space,
but for black holes, Unruh's sonic analogy has given rise to both field
theoretic and ... | [
{
"created": "Thu, 13 Jan 2000 23:55:48 GMT",
"version": "v1"
},
{
"created": "Wed, 16 Feb 2000 23:37:34 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Jacobson",
"Ted",
""
]
] | Trans-Planckian redshifts in cosmology and outside black holes may provide windows on a hypothetical short distance cutoff on the fundamental degrees of freedom. In cosmology, such a cutoff seems to require a growing Hilbert space, but for black holes, Unruh's sonic analogy has given rise to both field theoretic and la... | 12.339303 | 13.994425 | 11.856761 | 11.801633 | 12.147556 | 13.224023 | 13.097897 | 12.779846 | 11.789509 | 12.700234 | 12.645608 | 11.206047 | 12.051828 | 11.564852 | 11.621494 | 11.250927 | 11.578577 | 11.600391 | 11.573761 | 11.781324 | 12.038488 |
hep-th/0507235 | Lee Smolin | Lee Smolin | The case for background independence | Latex, 46 pages, no figures | null | null | null | hep-th | null | The aim of this paper is to explain carefully the arguments behind the
assertion that the correct quantum theory of gravity must be background
independent. We begin by recounting how the debate over whether quantum gravity
must be background independent is a continuation of a long-standing argument in
the history of ... | [
{
"created": "Mon, 25 Jul 2005 15:47:31 GMT",
"version": "v1"
}
] | 2007-05-23 | [
[
"Smolin",
"Lee",
""
]
] | The aim of this paper is to explain carefully the arguments behind the assertion that the correct quantum theory of gravity must be background independent. We begin by recounting how the debate over whether quantum gravity must be background independent is a continuation of a long-standing argument in the history of ph... | 7.805217 | 8.879899 | 8.970944 | 8.289386 | 8.571939 | 8.664135 | 8.487133 | 8.733925 | 8.094384 | 9.042871 | 7.914001 | 8.011139 | 8.109486 | 8.036737 | 8.163779 | 8.158443 | 8.549621 | 8.074535 | 8.140212 | 8.159638 | 7.964498 |
0804.0899 | Francesco Nitti | U.Gursoy, E.Kiritsis, L. Mazzanti, F.Nitti | Deconfinement and Gluon Plasma Dynamics in Improved Holographic QCD | LaTeX, 15 pages, 6 eps figures. Added comments and references;
corrected misprint in eq. (3.5). A slightly shorter version of this work will
appear in Physical Review Letters | Phys.Rev.Lett.101:181601,2008 | 10.1103/PhysRevLett.101.181601 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The finite temperature physics of the pure glue sector in the improved
holographic QCD model of arXiv:0707.1324 and arXiv:0707.1349 is addressed. The
thermodynamics of 5D dilaton gravity duals to confining gauge theories is
analyzed. We show that they exhibit a first order Hawking-Page type phase
transition. In the e... | [
{
"created": "Mon, 7 Apr 2008 17:25:24 GMT",
"version": "v1"
},
{
"created": "Tue, 8 Apr 2008 15:15:26 GMT",
"version": "v2"
},
{
"created": "Sat, 25 Oct 2008 08:52:55 GMT",
"version": "v3"
}
] | 2008-10-31 | [
[
"Gursoy",
"U.",
""
],
[
"Kiritsis",
"E.",
""
],
[
"Mazzanti",
"L.",
""
],
[
"Nitti",
"F.",
""
]
] | The finite temperature physics of the pure glue sector in the improved holographic QCD model of arXiv:0707.1324 and arXiv:0707.1349 is addressed. The thermodynamics of 5D dilaton gravity duals to confining gauge theories is analyzed. We show that they exhibit a first order Hawking-Page type phase transition. In the exp... | 6.808204 | 6.028995 | 6.616545 | 5.532151 | 6.284195 | 5.747297 | 6.197791 | 6.073333 | 5.33146 | 7.181501 | 6.09733 | 6.102735 | 6.174988 | 5.756386 | 5.953596 | 5.938642 | 6.020423 | 5.980732 | 5.841882 | 6.319393 | 6.167339 |
1505.02483 | Rodrigo Bufalo | R. Bufalo | Born-Infeld electrodynamics in very special relativity | 14 pages; to appear in PLB | Phys. Lett. B 746, 251 (2015) | 10.1016/j.physletb.2015.05.014 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we discuss the properties of a modified Born-Infeld
electrodynamics in the framework of very special relativity (VSR). This
proposal allows us to study VSR mass effects in a gauge-invariant context of
nonlinear electrodynamics. It is analyzed in detail the electrostatic solutions
for two different cases,... | [
{
"created": "Mon, 11 May 2015 05:17:25 GMT",
"version": "v1"
}
] | 2015-05-18 | [
[
"Bufalo",
"R.",
""
]
] | In this work we discuss the properties of a modified Born-Infeld electrodynamics in the framework of very special relativity (VSR). This proposal allows us to study VSR mass effects in a gauge-invariant context of nonlinear electrodynamics. It is analyzed in detail the electrostatic solutions for two different cases, a... | 9.860861 | 9.228487 | 9.108391 | 8.325098 | 8.410845 | 8.173856 | 8.767741 | 8.228151 | 8.364877 | 10.366179 | 8.843346 | 8.871081 | 8.832952 | 8.769693 | 8.834367 | 8.75242 | 8.759122 | 8.801918 | 8.788477 | 9.048722 | 9.081525 |
2207.10989 | Luis M. Nieto | A. Alonso-Izquierdo, D. Migu\'elez-Caballero, L. M. Nieto, and J.
Queiroga-Nunes | Wobbling kinks in a two-component scalar field theory: Interaction
between shape modes | 28 pages, 11 figures | null | 10.1016/j.physd.2022.133590 | null | hep-th math-ph math.MP nlin.PS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper the interaction between the shape modes of the wobbling kinks
arising in the family of two-component MSTB scalar field theory models is
studied. The spectrum of the second order small kink fluctuation in this model
has two localized vibrational modes associated to longitudinal and orthogonal
fluctuation... | [
{
"created": "Fri, 22 Jul 2022 10:11:46 GMT",
"version": "v1"
}
] | 2022-11-30 | [
[
"Alonso-Izquierdo",
"A.",
""
],
[
"Miguélez-Caballero",
"D.",
""
],
[
"Nieto",
"L. M.",
""
],
[
"Queiroga-Nunes",
"J.",
""
]
] | In this paper the interaction between the shape modes of the wobbling kinks arising in the family of two-component MSTB scalar field theory models is studied. The spectrum of the second order small kink fluctuation in this model has two localized vibrational modes associated to longitudinal and orthogonal fluctuations ... | 12.407992 | 11.529029 | 12.838675 | 10.772402 | 11.956335 | 10.745233 | 11.906252 | 11.927462 | 10.761574 | 13.809088 | 11.901388 | 10.95453 | 11.493072 | 11.048734 | 11.462625 | 11.592863 | 11.529329 | 11.320333 | 10.90343 | 11.718011 | 11.442714 |
hep-th/9803203 | Gary Gibbons | G W Gibbons | Branes as BIons | Latex, 9 pages, no figures | Class.Quant.Grav.16:1471-1477,1999 | 10.1088/0264-9381/16/5/301 | null | hep-th | null | A BIon may be defined as a finite energy solution of a non-linear field
theory with distributional sources. By contrast a soliton is usually defined to
have no sources. I show how harmonic coordinates map the exteriors of the
topologically and causally non-trivial spacetimes of extreme p-branes to BIonic
solutions of... | [
{
"created": "Wed, 25 Mar 1998 14:07:27 GMT",
"version": "v1"
}
] | 2009-10-07 | [
[
"Gibbons",
"G W",
""
]
] | A BIon may be defined as a finite energy solution of a non-linear field theory with distributional sources. By contrast a soliton is usually defined to have no sources. I show how harmonic coordinates map the exteriors of the topologically and causally non-trivial spacetimes of extreme p-branes to BIonic solutions of t... | 15.344714 | 15.097016 | 14.766563 | 12.56002 | 14.405161 | 13.664131 | 16.194574 | 13.672314 | 13.79528 | 16.379871 | 13.261611 | 12.759171 | 13.432912 | 12.719905 | 13.2959 | 13.43754 | 13.857917 | 12.918936 | 13.257689 | 14.434924 | 12.483582 |
1401.5414 | A. Yu. Petrov | F. S. Gama, M. Gomes, J. R. Nascimento, A. Yu. Petrov, A. J. da Silva | On the one-loop effective potential in the higher-derivative
four-dimensional chiral superfield theory with a nonconventional kinetic term | 9 pages | Phys. Lett. B733, 247 (2014) | 10.1016/j.physletb.2014.04.054 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly calculate the one-loop effective potential for a
higher-derivative four-dimensional chiral superfield theory with a
nonconventional kinetic term. We consider the cases of minimal and nonminimal
general Lagrangians. In particular, we find that in the minimal case the
divergent part of the one-loop effect... | [
{
"created": "Tue, 21 Jan 2014 18:23:13 GMT",
"version": "v1"
}
] | 2014-05-15 | [
[
"Gama",
"F. S.",
""
],
[
"Gomes",
"M.",
""
],
[
"Nascimento",
"J. R.",
""
],
[
"Petrov",
"A. Yu.",
""
],
[
"da Silva",
"A. J.",
""
]
] | We explicitly calculate the one-loop effective potential for a higher-derivative four-dimensional chiral superfield theory with a nonconventional kinetic term. We consider the cases of minimal and nonminimal general Lagrangians. In particular, we find that in the minimal case the divergent part of the one-loop effectiv... | 8.064083 | 7.447183 | 8.746436 | 7.176299 | 7.168664 | 7.44045 | 7.998166 | 7.715231 | 7.369432 | 9.094694 | 7.424578 | 7.272956 | 8.514567 | 7.616106 | 7.638542 | 7.445582 | 7.272668 | 7.201709 | 7.656894 | 8.365166 | 6.969643 |
2011.13981 | Soumyadeep Chaudhuri | Soumyadeep Chaudhuri, Changha Choi, Eliezer Rabinovici | Thermal order in large N conformal gauge theories | 116 pages, v4: typos have been corrected, comments and references
have been added, version matches with the published one | null | 10.1007/JHEP04(2021)203 | null | hep-th cond-mat.str-el hep-ph | http://creativecommons.org/licenses/by/4.0/ | In this work we explore the possibility of spontaneous breaking of global
symmetries at all nonzero temperatures for conformal field theories (CFTs) in
$D = 4$ space-time dimensions. We show that such a symmetry-breaking indeed
occurs in certain families of non-supersymmetric large $N$ gauge theories at a
planar limi... | [
{
"created": "Fri, 27 Nov 2020 20:20:14 GMT",
"version": "v1"
},
{
"created": "Tue, 12 Jan 2021 11:59:34 GMT",
"version": "v2"
},
{
"created": "Wed, 24 Feb 2021 02:46:28 GMT",
"version": "v3"
},
{
"created": "Tue, 20 Apr 2021 08:00:44 GMT",
"version": "v4"
}
] | 2021-05-12 | [
[
"Chaudhuri",
"Soumyadeep",
""
],
[
"Choi",
"Changha",
""
],
[
"Rabinovici",
"Eliezer",
""
]
] | In this work we explore the possibility of spontaneous breaking of global symmetries at all nonzero temperatures for conformal field theories (CFTs) in $D = 4$ space-time dimensions. We show that such a symmetry-breaking indeed occurs in certain families of non-supersymmetric large $N$ gauge theories at a planar limit.... | 6.960455 | 7.029261 | 7.188385 | 6.884875 | 7.4542 | 7.337093 | 6.930197 | 7.095609 | 6.850387 | 7.470642 | 6.94592 | 6.630528 | 6.978027 | 6.783357 | 6.76564 | 6.721386 | 6.78959 | 6.694981 | 6.819806 | 7.1757 | 6.600337 |
2009.13137 | Mikhail Goykhman | Mikhail Goykhman, Vladimir Rosenhaus, Michael Smolkin | The background field method and critical vector models | v2: references added (published version) | null | 10.1007/JHEP02(2021)074 | null | hep-th cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We use the background field method to systematically derive CFT data for the
critical $\phi^6$ vector model in three dimensions, and the Gross-Neveu model
in dimensions $2\leq d \leq 4$. Specifically, we calculate the OPE coefficients
and anomalous dimensions of various operators, up to next-to-leading order in
the $... | [
{
"created": "Mon, 28 Sep 2020 08:36:29 GMT",
"version": "v1"
},
{
"created": "Wed, 24 Feb 2021 13:25:48 GMT",
"version": "v2"
}
] | 2021-02-25 | [
[
"Goykhman",
"Mikhail",
""
],
[
"Rosenhaus",
"Vladimir",
""
],
[
"Smolkin",
"Michael",
""
]
] | We use the background field method to systematically derive CFT data for the critical $\phi^6$ vector model in three dimensions, and the Gross-Neveu model in dimensions $2\leq d \leq 4$. Specifically, we calculate the OPE coefficients and anomalous dimensions of various operators, up to next-to-leading order in the $1/... | 4.931013 | 4.082417 | 5.517622 | 4.276221 | 4.279735 | 4.039787 | 4.111112 | 4.140041 | 4.174252 | 5.960639 | 4.245331 | 4.343887 | 4.930533 | 4.320711 | 4.164913 | 4.30807 | 4.166567 | 4.431611 | 4.320457 | 4.724934 | 4.315095 |
hep-th/0307116 | Gernot Akemann | G. Akemann | Equivalence of Matrix Models for Complex QCD Dirac Spectra | 13 pages, 4 figures, references added | Acta Phys.Polon. B34 (2003) 4653-4666 | null | SPhT T03/103 | hep-th hep-lat hep-ph | null | Two different matrix models for QCD with a non-vanishing quark chemical
potential are shown to be equivalent by mapping the corresponding partition
functions. The equivalence holds in the phase with broken chiral symmetry. It
is exact in the limit of weak non-Hermiticity, where the chemical potential
squared is resca... | [
{
"created": "Sat, 12 Jul 2003 13:56:28 GMT",
"version": "v1"
},
{
"created": "Wed, 23 Jul 2003 09:53:42 GMT",
"version": "v2"
}
] | 2007-05-23 | [
[
"Akemann",
"G.",
""
]
] | Two different matrix models for QCD with a non-vanishing quark chemical potential are shown to be equivalent by mapping the corresponding partition functions. The equivalence holds in the phase with broken chiral symmetry. It is exact in the limit of weak non-Hermiticity, where the chemical potential squared is rescale... | 9.990823 | 9.899162 | 10.209637 | 8.631941 | 9.557592 | 9.174978 | 9.326765 | 8.941662 | 8.864938 | 11.344817 | 8.673762 | 9.016675 | 9.127362 | 9.093524 | 8.969323 | 9.101037 | 9.054996 | 9.370386 | 9.423018 | 10.063501 | 9.188558 |
hep-th/0010081 | Henrique Boschi-Filho | C. P. Natividade, H. Boschi-Filho and L. V. Belvedere | BFFT formalism applied to the minimal chiral Schwinger model | 11 Latex pages. Revised version: New section and more references
included. To appear in MPLA | Mod.Phys.Lett. A19 (2004) 2957 | 10.1142/S0217732304014069 | null | hep-th | null | We consider the minimal chiral Schwinger model, by embedding the gauge
noninvariant formulation into a gauge theory following the
Batalin-Fradkin-Fradkina-Tyutin point of view. Within the BFFT procedure, the
second class constraints are converted into strongly involutive first-class
ones, leading to an extended gauge... | [
{
"created": "Wed, 11 Oct 2000 13:53:00 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Dec 2000 19:05:44 GMT",
"version": "v2"
},
{
"created": "Thu, 16 Sep 2004 14:15:52 GMT",
"version": "v3"
}
] | 2007-05-23 | [
[
"Natividade",
"C. P.",
""
],
[
"Boschi-Filho",
"H.",
""
],
[
"Belvedere",
"L. V.",
""
]
] | We consider the minimal chiral Schwinger model, by embedding the gauge noninvariant formulation into a gauge theory following the Batalin-Fradkin-Fradkina-Tyutin point of view. Within the BFFT procedure, the second class constraints are converted into strongly involutive first-class ones, leading to an extended gauge i... | 10.820919 | 10.068373 | 13.484734 | 9.873969 | 9.179768 | 9.357084 | 10.345385 | 9.816113 | 9.285351 | 13.446308 | 8.826733 | 9.355602 | 11.439847 | 9.926529 | 9.379488 | 9.824326 | 9.725833 | 9.325857 | 9.959841 | 10.091586 | 9.661292 |
1203.1837 | Don N. Page | Don N. Page | Normalized Observational Probabilities from Unnormalizable Quantum
States or Phase-Space Distributions | 15 pages, LaTeX | null | null | Alberta Thy 5-12 | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Often it is assumed that a quantum state or a phase-space distribution must
be normalizable. Here it is shown that even if it is not normalizable, one may
be able to extract normalized observational probabilities from it.
| [
{
"created": "Thu, 8 Mar 2012 16:08:47 GMT",
"version": "v1"
}
] | 2012-03-09 | [
[
"Page",
"Don N.",
""
]
] | Often it is assumed that a quantum state or a phase-space distribution must be normalizable. Here it is shown that even if it is not normalizable, one may be able to extract normalized observational probabilities from it. | 13.568701 | 11.103526 | 11.64831 | 10.988308 | 11.755034 | 10.982369 | 12.084753 | 11.356622 | 10.932347 | 11.665861 | 11.344365 | 10.343537 | 11.28412 | 11.395465 | 10.71247 | 10.48089 | 10.297688 | 10.622512 | 11.05698 | 11.138162 | 11.640984 |
1301.4174 | Hossein Yavartanoo | Hossein Yavartanoo | EVH Black Hole Solutions With Higher Derivative Corrections | 15 pages | Eur.Phys.J. C72 (2012) 1911 | 10.1140/epjc/s10052-012-1911-7 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We analyze the effect of higher derivative corrections to the near horizon
geometry of the extremal vanishing horizon (EVH) black hole solutions in four
dimensions. We restrict ourselves to the Gauss-Bonnet correction with a
dilation dependent coupling in an Einstein Maxwell dilaton theory. This action
may represent ... | [
{
"created": "Thu, 17 Jan 2013 18:00:37 GMT",
"version": "v1"
}
] | 2013-01-18 | [
[
"Yavartanoo",
"Hossein",
""
]
] | We analyze the effect of higher derivative corrections to the near horizon geometry of the extremal vanishing horizon (EVH) black hole solutions in four dimensions. We restrict ourselves to the Gauss-Bonnet correction with a dilation dependent coupling in an Einstein Maxwell dilaton theory. This action may represent th... | 7.838563 | 6.459621 | 8.477206 | 6.90068 | 7.487838 | 6.658734 | 7.020003 | 6.846714 | 6.930577 | 9.373178 | 6.702981 | 7.272408 | 7.607601 | 7.065351 | 7.204587 | 7.178145 | 7.13435 | 7.112473 | 7.100334 | 7.844555 | 7.126758 |
hep-th/9603087 | Paul Townsend | G. Papadopoulos and P.K. Townsend | Intersecting M-branes | Derivation of an intersection rule added. Some additional refs.
Version accepted for publication in PLB. Phyzzx macro | Phys.Lett.B380:273-279,1996 | 10.1016/0370-2693(96)00506-0 | null | hep-th | null | We present the magnetic duals of G\"uven's electric-type solutions of D=11
supergravity preserving $1/4$ or $1/8$ of the D=11 supersymmetry. We interpret
the electric solutions as $n$ orthogonal intersecting membranes and the
magnetic solutions as $n$ orthogonal intersecting 5-branes, with $n=2,3$; these
cases obey t... | [
{
"created": "Wed, 13 Mar 1996 19:23:33 GMT",
"version": "v1"
},
{
"created": "Fri, 15 Mar 1996 18:44:03 GMT",
"version": "v2"
},
{
"created": "Mon, 29 Apr 1996 15:05:17 GMT",
"version": "v3"
}
] | 2009-10-09 | [
[
"Papadopoulos",
"G.",
""
],
[
"Townsend",
"P. K.",
""
]
] | We present the magnetic duals of G\"uven's electric-type solutions of D=11 supergravity preserving $1/4$ or $1/8$ of the D=11 supersymmetry. We interpret the electric solutions as $n$ orthogonal intersecting membranes and the magnetic solutions as $n$ orthogonal intersecting 5-branes, with $n=2,3$; these cases obey the... | 5.975709 | 5.702824 | 5.842565 | 5.434924 | 5.793724 | 5.324708 | 5.521102 | 5.407964 | 5.001358 | 6.149913 | 5.338274 | 5.511905 | 5.587124 | 5.810658 | 5.628101 | 5.637483 | 5.671299 | 5.615445 | 5.687107 | 5.543872 | 5.580962 |
2005.04178 | Pedro Alvarez | Pedro D. Alvarez, Mauricio Valenzuela and Jorge Zanelli | Chiral gauge theory and gravity from unconventional supersymmetry | 31 pages | null | 10.1007/JHEP07(2020)205 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | From a gauge $SU(2,2|2)$ model with broken supersymmetry, we construct an
action for $SU(2)\times U(1)$ Yang-Mills theory coupled to gravity and matter.
The connection components for AdS boosts and special conformal translations are
auxiliary fields and their fixing reduces the theory to two distintive sectors:
a vec... | [
{
"created": "Fri, 8 May 2020 17:16:35 GMT",
"version": "v1"
}
] | 2020-08-26 | [
[
"Alvarez",
"Pedro D.",
""
],
[
"Valenzuela",
"Mauricio",
""
],
[
"Zanelli",
"Jorge",
""
]
] | From a gauge $SU(2,2|2)$ model with broken supersymmetry, we construct an action for $SU(2)\times U(1)$ Yang-Mills theory coupled to gravity and matter. The connection components for AdS boosts and special conformal translations are auxiliary fields and their fixing reduces the theory to two distintive sectors: a vecto... | 14.927015 | 14.860977 | 13.343526 | 13.023036 | 15.40933 | 14.187849 | 15.307699 | 14.058374 | 13.390029 | 16.080946 | 14.625547 | 14.013566 | 12.872813 | 13.81163 | 14.544948 | 14.081572 | 14.176823 | 14.156803 | 13.425355 | 13.729848 | 13.298462 |
hep-th/0103100 | Yun S. Song | Jun Li, Yun S. Song | Open string instantons and relative stable morphisms | This is the version published by Geometry & Topology Monographs on 22
April 2006 | Adv.Theor.Math.Phys.5:67-91,2002 | 10.2140/gtm.2006.8.49 | null | hep-th math.AG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We show how topological open string theory amplitudes can be computed by
using relative stable morphisms in the algebraic category. We achieve our goal
by explicitly working through an example which has been previously considered
by Ooguri and Vafa from the point of view of physics. By using the method of
virtual loc... | [
{
"created": "Tue, 13 Mar 2001 22:54:55 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Apr 2001 20:21:36 GMT",
"version": "v2"
},
{
"created": "Tue, 24 Mar 2009 14:49:02 GMT",
"version": "v3"
},
{
"created": "Wed, 20 Jul 2011 04:01:26 GMT",
"version": "v4"
}
] | 2011-07-21 | [
[
"Li",
"Jun",
""
],
[
"Song",
"Yun S.",
""
]
] | We show how topological open string theory amplitudes can be computed by using relative stable morphisms in the algebraic category. We achieve our goal by explicitly working through an example which has been previously considered by Ooguri and Vafa from the point of view of physics. By using the method of virtual local... | 7.102913 | 7.200742 | 9.227846 | 7.270368 | 7.489608 | 7.595143 | 7.64665 | 7.101213 | 6.980638 | 8.675986 | 6.987099 | 6.935744 | 8.034648 | 7.224585 | 7.183345 | 7.158917 | 7.03206 | 6.957909 | 6.676787 | 7.724905 | 6.914537 |
1903.03789 | Stefan Groot Nibbelink | Stefan Groot Nibbelink | Nonexistence of locally but not globally supersymmetric orbifolds | 8 pages LaTeX | null | 10.1088/1742-6596/1586/1/012030 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Motivated by the smallness of the cosmological constant we investigate
whether it is possible to have vanishing one-loop heterotic string partition
functions for six-dimensional non-supersymmetric toroidal orbifolds. A
straightforward way to realize this presents itself, when each orbifold sector
separately preserves... | [
{
"created": "Sat, 9 Mar 2019 12:22:37 GMT",
"version": "v1"
}
] | 2020-12-30 | [
[
"Nibbelink",
"Stefan Groot",
""
]
] | Motivated by the smallness of the cosmological constant we investigate whether it is possible to have vanishing one-loop heterotic string partition functions for six-dimensional non-supersymmetric toroidal orbifolds. A straightforward way to realize this presents itself, when each orbifold sector separately preserves s... | 14.313875 | 13.317423 | 15.509489 | 12.646222 | 14.59411 | 15.551122 | 14.436386 | 14.762762 | 13.037214 | 15.527246 | 13.469879 | 12.576456 | 12.893396 | 12.594313 | 13.17596 | 13.108828 | 13.092748 | 13.033957 | 13.443696 | 13.515243 | 12.628018 |
hep-th/0506110 | David Mateos | Roberto Emparan and David Mateos | Oscillator Level for Black Holes and Black Rings | 14 pages; v2: Distinction between near-horizon and full BTZ metrics
clarified, reference added | Class.Quant.Grav. 22 (2005) 3575-3584 | 10.1088/0264-9381/22/17/016 | null | hep-th | null | Microscopic calculations of the Bekenstein-Hawking entropy of supersymmetric
black holes in string theory are typically based on the application to a dual
2D CFT of Cardy's formula, S=2\pi \sqrt{c q /6}, where `c' is the central
charge and `q' is the oscillator level. In the CFT, q is non-trivially related
to the tot... | [
{
"created": "Tue, 14 Jun 2005 19:54:36 GMT",
"version": "v1"
},
{
"created": "Wed, 29 Jun 2005 18:03:52 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Emparan",
"Roberto",
""
],
[
"Mateos",
"David",
""
]
] | Microscopic calculations of the Bekenstein-Hawking entropy of supersymmetric black holes in string theory are typically based on the application to a dual 2D CFT of Cardy's formula, S=2\pi \sqrt{c q /6}, where `c' is the central charge and `q' is the oscillator level. In the CFT, q is non-trivially related to the total... | 8.316376 | 7.422167 | 8.398737 | 7.636045 | 7.242727 | 7.791117 | 7.57257 | 7.368836 | 7.331059 | 9.791133 | 7.021356 | 7.087844 | 7.541519 | 6.987967 | 7.62407 | 7.037476 | 7.380994 | 6.820695 | 6.89586 | 8.197765 | 6.985081 |
1911.08601 | Dine Ousmane Samary | Vincent Lahoche and Dine Ousmane Samary | Large-$d$ behavior of the Feynman amplitudes for a just-renormalizable
tensorial group field theory | 50 pages 5 figures | Phys. Rev. D 103, 085006 (2021) | 10.1103/PhysRevD.103.085006 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper aims at giving a novel approach to investigate the behavior of the
renormalization group flow for tensorial group field theories to all orders of
the perturbation theory. From an appropriate choice of the kinetic kernel, we
build an infinite family of just-renormalizable models, for tensor fields with
arbi... | [
{
"created": "Tue, 19 Nov 2019 21:42:40 GMT",
"version": "v1"
},
{
"created": "Wed, 1 Mar 2023 19:41:23 GMT",
"version": "v2"
}
] | 2023-03-03 | [
[
"Lahoche",
"Vincent",
""
],
[
"Samary",
"Dine Ousmane",
""
]
] | This paper aims at giving a novel approach to investigate the behavior of the renormalization group flow for tensorial group field theories to all orders of the perturbation theory. From an appropriate choice of the kinetic kernel, we build an infinite family of just-renormalizable models, for tensor fields with arbitr... | 11.853059 | 11.720081 | 12.053245 | 10.335427 | 11.958085 | 11.943409 | 11.777392 | 11.259149 | 10.869395 | 13.214108 | 11.088553 | 11.250014 | 11.697534 | 11.318986 | 11.42451 | 11.574643 | 11.261291 | 11.02563 | 11.567724 | 11.99734 | 11.000494 |
hep-th/0510044 | Eva Silverstein | Eva Silverstein | Dimensional Mutation and Spacelike Singularities | 15 pages, harvmac big. v2: 18 pages, harvmac big; added computation
of density of states and modular invariance check, enhanced discussion of
multiplicity of solutions all sharing the feature of increased density of
states, added references | Phys.Rev.D73:086004,2006 | 10.1103/PhysRevD.73.086004 | SU-ITP-05/26 SLAC-PUB-11510 | hep-th | null | I argue that string theory compactified on a Riemann surface crosses over at
small volume to a higher dimensional background of supercritical string theory.
Several concrete measures of the count of degrees of freedom of the theory
yield the consistent result that at finite volume, the effective dimensionality
is inc... | [
{
"created": "Wed, 5 Oct 2005 17:44:22 GMT",
"version": "v1"
},
{
"created": "Mon, 27 Feb 2006 01:45:35 GMT",
"version": "v2"
}
] | 2008-11-26 | [
[
"Silverstein",
"Eva",
""
]
] | I argue that string theory compactified on a Riemann surface crosses over at small volume to a higher dimensional background of supercritical string theory. Several concrete measures of the count of degrees of freedom of the theory yield the consistent result that at finite volume, the effective dimensionality is incre... | 14.458919 | 15.784945 | 14.526158 | 13.993761 | 15.558869 | 15.522521 | 16.130419 | 14.391187 | 15.12816 | 16.476976 | 13.922494 | 13.554623 | 14.142629 | 13.682932 | 14.300211 | 13.908941 | 14.221934 | 13.591219 | 13.632642 | 14.234109 | 13.598405 |
hep-th/0507012 | Stefan Zohren | R. Loll (U. Utrecht), W. Westra (U. Utrecht), S. Zohren (U. Utrecht,
RWTH Aachen) | Taming the cosmological constant in 2D causal quantum gravity with
topology change | 19 pages, 4 figures. Comments on general covariance added. To be
published in Nucl. Phys. B | Nucl.Phys. B751 (2006) 419-435 | 10.1016/j.nuclphysb.2006.06.033 | null | hep-th | null | As shown in previous work, there is a well-defined nonperturbative
gravitational path integral including an explicit sum over topologies in the
setting of Causal Dynamical Triangulations in two dimensions. In this paper we
derive a complete analytical solution of the quantum continuum dynamics of this
model, obtained... | [
{
"created": "Fri, 1 Jul 2005 13:50:51 GMT",
"version": "v1"
},
{
"created": "Tue, 27 Jun 2006 11:53:43 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Loll",
"R.",
"",
"U. Utrecht"
],
[
"Westra",
"W.",
"",
"U. Utrecht"
],
[
"Zohren",
"S.",
"",
"U. Utrecht,\n RWTH Aachen"
]
] | As shown in previous work, there is a well-defined nonperturbative gravitational path integral including an explicit sum over topologies in the setting of Causal Dynamical Triangulations in two dimensions. In this paper we derive a complete analytical solution of the quantum continuum dynamics of this model, obtained u... | 10.945418 | 9.332878 | 9.704174 | 8.967412 | 8.916963 | 9.7256 | 9.038772 | 8.818428 | 9.565015 | 11.274541 | 10.014944 | 9.717034 | 10.515612 | 10.015078 | 9.693294 | 9.91709 | 9.584698 | 9.666626 | 10.121064 | 10.189225 | 9.960332 |
0801.3949 | Hugo Looyestijn | Hugo Looyestijn and Stefan Vandoren | On NS5-brane instantons and volume stabilization | 29 pages, 3 figures; statements about fields G^a made more precise,
added some clarifications, typos corrected | JHEP 0804:024,2008 | 10.1088/1126-6708/2008/04/024 | null | hep-th | null | We study general aspects of NS5-brane instantons in relation to the
stabilization of the volume modulus in Calabi-Yau compactifications of type II
strings with fluxes, and their orientifold versions. These instantons correct
the Kahler potential and generically yield significant contributions to the
scalar potential ... | [
{
"created": "Fri, 25 Jan 2008 14:46:40 GMT",
"version": "v1"
},
{
"created": "Sun, 27 Jan 2008 08:29:48 GMT",
"version": "v2"
},
{
"created": "Wed, 20 Feb 2008 08:32:35 GMT",
"version": "v3"
}
] | 2014-11-18 | [
[
"Looyestijn",
"Hugo",
""
],
[
"Vandoren",
"Stefan",
""
]
] | We study general aspects of NS5-brane instantons in relation to the stabilization of the volume modulus in Calabi-Yau compactifications of type II strings with fluxes, and their orientifold versions. These instantons correct the Kahler potential and generically yield significant contributions to the scalar potential at... | 10.487522 | 8.750745 | 10.838094 | 9.372846 | 10.371875 | 9.040642 | 10.112378 | 9.076685 | 9.10518 | 12.273939 | 9.037565 | 9.62437 | 10.656852 | 9.833962 | 9.689222 | 9.679126 | 10.142504 | 9.696735 | 9.465424 | 9.585653 | 9.510351 |
1408.0425 | Alexey Milekhin | A. Gorsky, A. Milekhin | RG-Whitham dynamics and complex Hamiltonian systems | v3: 34 pages, several typos corrected, a reference added, to appear
in Nuclear Physics B | null | 10.1016/j.nuclphysb.2015.03.028 | ITEP-TH-19/14 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Inspired by the Seiberg-Witten exact solution, we consider some aspects of
the Hamiltonian dynamics with the complexified phase space focusing at the
renormalization group(RG)-like Whitham behavior. We show that at the
Argyres-Douglas(AD) point the number of degrees of freedom in Hamiltonian
system effectively reduce... | [
{
"created": "Sat, 2 Aug 2014 21:40:57 GMT",
"version": "v1"
},
{
"created": "Sun, 16 Nov 2014 16:28:10 GMT",
"version": "v2"
},
{
"created": "Tue, 7 Apr 2015 12:20:22 GMT",
"version": "v3"
}
] | 2015-04-08 | [
[
"Gorsky",
"A.",
""
],
[
"Milekhin",
"A.",
""
]
] | Inspired by the Seiberg-Witten exact solution, we consider some aspects of the Hamiltonian dynamics with the complexified phase space focusing at the renormalization group(RG)-like Whitham behavior. We show that at the Argyres-Douglas(AD) point the number of degrees of freedom in Hamiltonian system effectively reduces ... | 12.797767 | 12.343113 | 14.754978 | 13.179824 | 12.710416 | 12.300056 | 12.412774 | 12.942653 | 13.163293 | 16.714102 | 12.624103 | 13.014736 | 14.113616 | 13.057265 | 13.027523 | 13.131396 | 12.481441 | 12.768438 | 13.159099 | 13.914451 | 12.791837 |
2210.11365 | Teresa Bautista | Teresa Bautista and Lorenzo Casarin | ANEC on stress-tensor states in perturbative $\lambda\phi^4$ theory | 25 pages | null | 10.1007/JHEP01(2023)097 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We evaluate the Average Null Energy Condition (ANEC) on momentum eigenstates
generated by the stress tensor in perturbative $\lambda \, \phi^4$ and general
spacetime dimension. We first compute the norm of the stress-tensor state at
second order in $\lambda$; as a by-product of the derivation we obtain the full
expre... | [
{
"created": "Thu, 20 Oct 2022 15:58:16 GMT",
"version": "v1"
}
] | 2023-02-08 | [
[
"Bautista",
"Teresa",
""
],
[
"Casarin",
"Lorenzo",
""
]
] | We evaluate the Average Null Energy Condition (ANEC) on momentum eigenstates generated by the stress tensor in perturbative $\lambda \, \phi^4$ and general spacetime dimension. We first compute the norm of the stress-tensor state at second order in $\lambda$; as a by-product of the derivation we obtain the full express... | 8.117194 | 7.835174 | 8.362438 | 7.295605 | 8.573799 | 8.173445 | 8.046485 | 7.711649 | 7.502719 | 8.777004 | 7.599137 | 8.350603 | 7.999083 | 7.471744 | 7.554421 | 7.569173 | 7.770629 | 7.548983 | 7.708263 | 8.153772 | 7.627557 |
1303.0755 | Eugenio R. Bezerra de Mello | E. R. Bezerra de Mello, E. R. Figueiredo Medeiros and A. A. Saharian | Fermionic vacuum polarization by a cosmic string in anti-de Sitter
spacetime | Appendix is added about the boundary condition on AdS boundary,
discussion and references are added related to AdS/CFT correspondence;
accepted for publication in Classical and Quantum Gravity | null | 10.1088/0264-9381/30/17/175001 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we investigate the fermionic condensate (FC) and the vacuum
expectation value (VEV) of the energy-momentum tensor, associated with a
massive fermionic field, induced by the presence of a cosmic string in the
anti-de Sitter (AdS) spacetime. In order to develop this analysis we construct
the complete set ... | [
{
"created": "Mon, 4 Mar 2013 16:58:04 GMT",
"version": "v1"
},
{
"created": "Thu, 4 Jul 2013 13:53:57 GMT",
"version": "v2"
}
] | 2015-06-15 | [
[
"de Mello",
"E. R. Bezerra",
""
],
[
"Medeiros",
"E. R. Figueiredo",
""
],
[
"Saharian",
"A. A.",
""
]
] | In this paper we investigate the fermionic condensate (FC) and the vacuum expectation value (VEV) of the energy-momentum tensor, associated with a massive fermionic field, induced by the presence of a cosmic string in the anti-de Sitter (AdS) spacetime. In order to develop this analysis we construct the complete set of... | 5.293553 | 3.502204 | 5.727004 | 3.97119 | 4.150821 | 3.732227 | 3.408424 | 3.856462 | 3.88374 | 5.869609 | 4.080458 | 4.603614 | 5.385835 | 4.886237 | 4.79632 | 4.662074 | 4.612204 | 4.623551 | 4.830587 | 5.458178 | 4.723438 |
2108.00016 | William Biggs | William D. Biggs and Jorge E. Santos | Rotating black holes in Randall-Sundrum II braneworlds | 6 pages, 4 figures | null | 10.1103/PhysRevLett.128.021601 | null | hep-th gr-qc hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We find rotating black hole solutions in the Randall-Sundrum II (RSII) model,
by numerically solving a three-dimensional PDE problem using pseudospectral
collocation methods. We compute the area and equatorial inner-most stable
orbits of these solutions. For large black holes compared with the AdS length
scale, $\ell... | [
{
"created": "Fri, 30 Jul 2021 18:00:02 GMT",
"version": "v1"
}
] | 2022-01-19 | [
[
"Biggs",
"William D.",
""
],
[
"Santos",
"Jorge E.",
""
]
] | We find rotating black hole solutions in the Randall-Sundrum II (RSII) model, by numerically solving a three-dimensional PDE problem using pseudospectral collocation methods. We compute the area and equatorial inner-most stable orbits of these solutions. For large black holes compared with the AdS length scale, $\ell$,... | 9.49441 | 9.518579 | 9.711872 | 8.828803 | 9.954432 | 9.408277 | 9.392097 | 10.141274 | 8.977059 | 10.708073 | 9.122993 | 9.076736 | 9.470953 | 9.046002 | 9.063001 | 8.996229 | 8.855914 | 9.143757 | 9.347524 | 9.2678 | 9.280213 |
1707.05274 | Eric R. Sharpe | W. Gu, E. Sharpe | A proposal for (0,2) mirrors of toric varieties | 52 pages, LaTeX; v2: miscellaneous writing updates, typos fixed | JHEP 1711 (2017) 112 | 10.1007/JHEP11(2017)112 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we propose (0,2) mirrors for general Fano toric varieties with
special tangent bundle deformations, corresponding to subsets of toric
deformations. Our mirrors are of the form of (B/2-twisted) (0,2)
Landau-Ginzburg models, matching Hori-Vafa mirrors on the (2,2) locus. We
compare our predictions to (0,2... | [
{
"created": "Mon, 17 Jul 2017 16:44:55 GMT",
"version": "v1"
},
{
"created": "Thu, 26 Oct 2017 22:24:09 GMT",
"version": "v2"
}
] | 2017-12-04 | [
[
"Gu",
"W.",
""
],
[
"Sharpe",
"E.",
""
]
] | In this paper we propose (0,2) mirrors for general Fano toric varieties with special tangent bundle deformations, corresponding to subsets of toric deformations. Our mirrors are of the form of (B/2-twisted) (0,2) Landau-Ginzburg models, matching Hori-Vafa mirrors on the (2,2) locus. We compare our predictions to (0,2) ... | 10.394631 | 10.200109 | 13.215818 | 9.876782 | 9.533762 | 9.666631 | 9.780513 | 10.192741 | 9.733181 | 14.19413 | 10.272041 | 9.752322 | 11.203801 | 9.468161 | 9.674392 | 9.788196 | 9.374676 | 9.573467 | 9.519198 | 10.791023 | 9.181993 |
1408.4066 | Jaime Besprosvany | J. Besprosvany and R. Romero | Representation of quantum field theory in an extended spin space and
fermion mass hierarchy | 23 pages, 5 tables. To be published in the Int. J. Mod. Phys. A | International Journal of Modern Physics A Vol. 29 (2014) 1450144
(17 pages) | 10.1142/S0217751X14501449 | null | hep-th hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider a matrix space based on the spin degree of freedom, describing
both a Hilbert state space, and its corresponding symmetry operators. Under the
requirement that the Lorentz symmetry be kept, at given dimension, scalar
symmetries, and their representations are determined. Symmetries are flavor or
gauge-like... | [
{
"created": "Mon, 18 Aug 2014 17:25:23 GMT",
"version": "v1"
}
] | 2015-12-17 | [
[
"Besprosvany",
"J.",
""
],
[
"Romero",
"R.",
""
]
] | We consider a matrix space based on the spin degree of freedom, describing both a Hilbert state space, and its corresponding symmetry operators. Under the requirement that the Lorentz symmetry be kept, at given dimension, scalar symmetries, and their representations are determined. Symmetries are flavor or gauge-like, ... | 22.857252 | 25.21623 | 22.635998 | 22.980909 | 24.762327 | 25.224173 | 24.830994 | 25.663256 | 23.355209 | 25.110142 | 22.562395 | 23.1542 | 22.505024 | 23.097425 | 23.408916 | 22.823303 | 24.064058 | 22.883223 | 22.642529 | 22.975651 | 22.125973 |
hep-th/9702117 | Dr Tsou Sheung Tsun | H. M. Chan (Rutherford Appleton Laboratory) and S. T. Tsou
(Mathematical Institute, Oxford University) | 't Hooft's Order-Disorder Parameters and the Dual Potential | Latex, 7 pages, no figures | Phys.Rev. D56 (1997) 3646-3649 | 10.1103/PhysRevD.56.3646 | RAL-TR-97-014 | hep-th | null | It is shown that the operator $B(C) = Tr [P \exp i \tilde{g} \oint
\tilde{A}_i(x) dx^i]$ constructed with the recently derived dual potential
$\tilde{A}(x)$ and a coupling $\tilde{g}$ related to $g$ by the Dirac
quantization condition satisfies the correct commutation relation with the
Wilson operator $Tr [P \exp ig ... | [
{
"created": "Fri, 14 Feb 1997 16:12:52 GMT",
"version": "v1"
}
] | 2016-09-06 | [
[
"Chan",
"H. M.",
"",
"Rutherford Appleton Laboratory"
],
[
"Tsou",
"S. T.",
"",
"Mathematical Institute, Oxford University"
]
] | It is shown that the operator $B(C) = Tr [P \exp i \tilde{g} \oint \tilde{A}_i(x) dx^i]$ constructed with the recently derived dual potential $\tilde{A}(x)$ and a coupling $\tilde{g}$ related to $g$ by the Dirac quantization condition satisfies the correct commutation relation with the Wilson operator $Tr [P \exp ig \o... | 8.141259 | 8.61147 | 7.736447 | 7.507468 | 7.616673 | 7.757233 | 7.60913 | 7.069659 | 6.843405 | 9.262865 | 6.904336 | 6.907188 | 6.551813 | 6.712957 | 6.862341 | 6.690992 | 6.755582 | 6.98677 | 6.775997 | 7.208739 | 6.895322 |
1612.05580 | Robert Shrock | Gongjun Choi, Thomas Ryttov, and Robert Shrock | On the Question of a Possible Infrared Zero in the Beta Function of the
Finite-$N$ Gross-Neveu Model | 10 pages | Phys. Rev. D 95, 025012 (2017) | 10.1103/PhysRevD.95.025012 | YITP-SB-2016-50, CP3-ORIGINS-2016-055-DNRF90 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate whether the beta function of the finite-$N$ Gross-Neveu model,
as calculated up to the four-loop level, exhibits evidence for an infrared
zero. As part of our analysis, we calculate and analyze Pad\'e approximants to
this beta function and evaluate effects of scheme dependence. From our study,
we find ... | [
{
"created": "Fri, 16 Dec 2016 18:24:06 GMT",
"version": "v1"
}
] | 2017-01-25 | [
[
"Choi",
"Gongjun",
""
],
[
"Ryttov",
"Thomas",
""
],
[
"Shrock",
"Robert",
""
]
] | We investigate whether the beta function of the finite-$N$ Gross-Neveu model, as calculated up to the four-loop level, exhibits evidence for an infrared zero. As part of our analysis, we calculate and analyze Pad\'e approximants to this beta function and evaluate effects of scheme dependence. From our study, we find th... | 8.225372 | 7.918702 | 8.125755 | 7.584423 | 7.462196 | 7.036381 | 7.71378 | 7.833325 | 7.237038 | 7.726547 | 6.96314 | 7.606522 | 7.684172 | 7.854641 | 7.698276 | 7.61454 | 7.888648 | 7.682183 | 7.585021 | 7.570879 | 7.504497 |
1708.07479 | Andrei Mironov | A. Mironov, A. Morozov | q-Painleve equation from Virasoro constraints | 6 pages | Phys.Lett. B785 (2018) 207-210 | 10.1016/j.physletb.2018.08.046 | FIAN/TD-17/17; IITP/TH-13/17; ITEP/TH-22/17 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The q-Painleve equation, satisfied by the Fourier transform of the q-Virasoro
conformal blocks at c=1, is interpreted as a reformulation of the string
equation and two other Virasoro constraints in the $5d$ Dotsenko-Fateev matrix
model.
| [
{
"created": "Thu, 24 Aug 2017 16:13:41 GMT",
"version": "v1"
}
] | 2018-09-05 | [
[
"Mironov",
"A.",
""
],
[
"Morozov",
"A.",
""
]
] | The q-Painleve equation, satisfied by the Fourier transform of the q-Virasoro conformal blocks at c=1, is interpreted as a reformulation of the string equation and two other Virasoro constraints in the $5d$ Dotsenko-Fateev matrix model. | 11.024503 | 9.465752 | 11.916609 | 9.721331 | 10.544729 | 8.342847 | 8.898607 | 9.390599 | 9.275665 | 15.232483 | 8.993538 | 9.319192 | 11.092573 | 9.371789 | 10.208627 | 9.707437 | 9.57923 | 9.85817 | 9.632026 | 11.688645 | 9.850848 |
hep-th/0403229 | Eloy Ay\'on-Beato | Eloy Ay\'on-Beato and Alberto Garc\'ia | Four Parametric Regular Black Hole Solution | RevTeX, 6 pages, minor changes | Gen.Rel.Grav. 37 (2005) 635 | 10.1007/s10714-005-0050-y | CECS-PHY-04/06 | hep-th gr-qc | null | We present a regular class of exact black hole solutions of Einstein
equations coupled with a nonlinear electrodynamics source. For weak fields the
nonlinear electrodynamics becomes the Maxwell theory, and asymptotically the
solutions behave as the Reissner-Nordstr\"om one. The class is endowed with
four parameters, ... | [
{
"created": "Tue, 23 Mar 2004 02:26:58 GMT",
"version": "v1"
},
{
"created": "Thu, 5 May 2005 17:29:38 GMT",
"version": "v2"
}
] | 2016-08-16 | [
[
"Ayón-Beato",
"Eloy",
""
],
[
"García",
"Alberto",
""
]
] | We present a regular class of exact black hole solutions of Einstein equations coupled with a nonlinear electrodynamics source. For weak fields the nonlinear electrodynamics becomes the Maxwell theory, and asymptotically the solutions behave as the Reissner-Nordstr\"om one. The class is endowed with four parameters, wh... | 5.704586 | 5.541109 | 4.729055 | 4.857453 | 5.044702 | 5.333892 | 5.482171 | 5.093888 | 5.187247 | 5.324618 | 5.463341 | 5.368279 | 5.127216 | 5.242964 | 5.222585 | 5.371115 | 5.420679 | 5.11474 | 5.462387 | 5.108036 | 5.343399 |
hep-th/9511133 | Giovanni Amelino | G. Amelino-Camelia, L. Griguolo, and D. Seminara | Lorentz Anomaly and 1+1-Dimensional Radiating Black Holes | 7 pages, LaTex | Phys.Lett. B371 (1996) 41-45 | 10.1016/0370-2693(95)01613-9 | OUTP-95-42-P/MIT-CTP-2484 | hep-th | null | The radiation from the black holes of a 1+1-dimensional chiral quantum
gravity model is studied. Most notably, a non-trivial dependence on a
renormalization parameter that characterizes the anomaly relations is uncovered
in an improved semiclassical approximation scheme; this dependence is not
present in the naive se... | [
{
"created": "Sat, 18 Nov 1995 16:07:00 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Amelino-Camelia",
"G.",
""
],
[
"Griguolo",
"L.",
""
],
[
"Seminara",
"D.",
""
]
] | The radiation from the black holes of a 1+1-dimensional chiral quantum gravity model is studied. Most notably, a non-trivial dependence on a renormalization parameter that characterizes the anomaly relations is uncovered in an improved semiclassical approximation scheme; this dependence is not present in the naive semi... | 17.857697 | 15.564055 | 16.062344 | 15.920197 | 16.130888 | 17.081442 | 15.278122 | 15.373442 | 15.891297 | 15.024462 | 15.562939 | 15.102114 | 16.280378 | 15.284938 | 14.428717 | 16.045858 | 15.142213 | 15.25447 | 15.41532 | 15.545131 | 14.930408 |
0704.2237 | Nadav Drukker | Nadav Drukker, Simone Giombi, Riccardo Ricci and Diego Trancanelli | More supersymmetric Wilson loops | 9 pages, LaTeX | Phys.Rev.D76:107703,2007 | 10.1103/PhysRevD.76.107703 | HU-EP-07/13, YITP-SB-07-12, Imperial/TP/07/RR/02 | hep-th | null | We present a large new family of Wilson loop operators in N=4 supersymmetric
Yang-Mills theory. For an arbitrary curve on the three dimensional sphere one
can add certain scalar couplings to the Wilson loop so it preserves at least
two supercharges. Some previously known loops, notably the 1/2 BPS circle,
belong to t... | [
{
"created": "Wed, 18 Apr 2007 14:25:53 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Drukker",
"Nadav",
""
],
[
"Giombi",
"Simone",
""
],
[
"Ricci",
"Riccardo",
""
],
[
"Trancanelli",
"Diego",
""
]
] | We present a large new family of Wilson loop operators in N=4 supersymmetric Yang-Mills theory. For an arbitrary curve on the three dimensional sphere one can add certain scalar couplings to the Wilson loop so it preserves at least two supercharges. Some previously known loops, notably the 1/2 BPS circle, belong to thi... | 9.724903 | 6.744739 | 11.072616 | 7.719305 | 7.642615 | 7.469979 | 6.77297 | 7.358971 | 7.684031 | 12.588994 | 7.738709 | 8.216303 | 9.744133 | 8.834904 | 8.952168 | 8.329186 | 8.626728 | 8.354014 | 8.925245 | 9.82424 | 9.212088 |
hep-th/9503210 | Louise Dolan | L. Dolan and S. Horvath | BRST properties of spin fields | 24 pages, plain tex, no figures | Nucl.Phys.B448:220-244,1995 | 10.1016/0550-3213(95)00251-M | IFP/499/UNC | hep-th | null | For the closed superstring, spin fields and bi-spinor states are defined
directly in four spacetime dimensions. Explicit operator product expansions are
given, including those for the internal superconformal field theory, which are
consistent with locality and BRST invariance for the string vertices. The most
general... | [
{
"created": "Wed, 29 Mar 1995 20:42:46 GMT",
"version": "v1"
}
] | 2010-11-15 | [
[
"Dolan",
"L.",
""
],
[
"Horvath",
"S.",
""
]
] | For the closed superstring, spin fields and bi-spinor states are defined directly in four spacetime dimensions. Explicit operator product expansions are given, including those for the internal superconformal field theory, which are consistent with locality and BRST invariance for the string vertices. The most general B... | 18.246975 | 17.52553 | 19.21295 | 16.2782 | 17.109236 | 17.15715 | 16.521395 | 17.168823 | 17.068607 | 21.220907 | 15.853515 | 16.860233 | 18.5576 | 17.678568 | 16.817995 | 17.478506 | 17.029034 | 16.959888 | 17.340897 | 19.080286 | 16.754093 |
0706.2050 | Georgi Dvali | Gia Dvali | Black Holes and Large N Species Solution to the Hierarchy Problem | 13 pages, Latex | Fortsch.Phys.58:528-536,2010 | 10.1002/prop.201000009 | null | hep-th | null | We provide the perturbative and non-perturbative arguments showing that
theories with large number of species of the quantum fields, imply an
inevitable hierarchy between the masses of the species and the Planck scale,
shedding a different light on the hierarchy problem. In particular, using the
black hole physics, w... | [
{
"created": "Thu, 14 Jun 2007 07:30:55 GMT",
"version": "v1"
}
] | 2014-11-18 | [
[
"Dvali",
"Gia",
""
]
] | We provide the perturbative and non-perturbative arguments showing that theories with large number of species of the quantum fields, imply an inevitable hierarchy between the masses of the species and the Planck scale, shedding a different light on the hierarchy problem. In particular, using the black hole physics, we ... | 12.206017 | 12.129211 | 12.613205 | 11.76429 | 12.907475 | 12.592935 | 12.984022 | 12.229055 | 11.392077 | 12.943162 | 11.76164 | 11.640357 | 11.636443 | 11.305821 | 11.097168 | 11.661607 | 11.387765 | 11.63383 | 11.345981 | 11.633087 | 11.131884 |
1703.05408 | Masaya Kameyama | Masaya Kameyama and Satoshi Nawata | Refined large N duality for knots | Two Mathematica notebooks are attached as ancillary files; in v2, the
title is changed, an extension to non-torus knots is included in section 6,
typos are corrected, and references are added; v3, published version | null | 10.1142/S0218216520410011 | CALT-2017-010 | hep-th math-ph math.AG math.GT math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We formulate large $N$ duality of $\mathrm{U}(N)$ refined Chern-Simons theory
with a torus knot/link in $S^3$. By studying refined BPS states in M-theory, we
provide the explicit form of low-energy effective actions of Type IIA string
theory with D4-branes on the $\Omega$-background. This form enables us to
relate re... | [
{
"created": "Wed, 15 Mar 2017 22:31:25 GMT",
"version": "v1"
},
{
"created": "Wed, 7 Jun 2017 13:46:26 GMT",
"version": "v2"
},
{
"created": "Wed, 15 Jul 2020 12:00:39 GMT",
"version": "v3"
}
] | 2020-07-16 | [
[
"Kameyama",
"Masaya",
""
],
[
"Nawata",
"Satoshi",
""
]
] | We formulate large $N$ duality of $\mathrm{U}(N)$ refined Chern-Simons theory with a torus knot/link in $S^3$. By studying refined BPS states in M-theory, we provide the explicit form of low-energy effective actions of Type IIA string theory with D4-branes on the $\Omega$-background. This form enables us to relate refi... | 5.979929 | 5.640745 | 7.496525 | 5.85926 | 5.943199 | 5.787252 | 5.863731 | 5.908176 | 5.766998 | 8.454332 | 5.611617 | 5.866791 | 6.61546 | 5.923998 | 5.692631 | 5.898291 | 5.836811 | 5.644584 | 5.831285 | 6.450832 | 5.785583 |
2311.12105 | Thibaut Coudarchet | Thibaut Coudarchet | Hiding the extra dimensions: A review on scale separation in string
theory | 1+63 pages, 3 figures. v2,v3: minor changes, references added | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present an overview of both older and recent developments concerning scale
separation in string theory. We focus on parametric scale separation obtained
at the classical level in flux compactifications down to AdS vacua. We review
the scenarios that have been proposed to achieve a hierarchy of scales between
space... | [
{
"created": "Mon, 20 Nov 2023 19:00:03 GMT",
"version": "v1"
},
{
"created": "Fri, 1 Dec 2023 16:33:41 GMT",
"version": "v2"
},
{
"created": "Mon, 19 Feb 2024 14:28:03 GMT",
"version": "v3"
}
] | 2024-02-20 | [
[
"Coudarchet",
"Thibaut",
""
]
] | We present an overview of both older and recent developments concerning scale separation in string theory. We focus on parametric scale separation obtained at the classical level in flux compactifications down to AdS vacua. We review the scenarios that have been proposed to achieve a hierarchy of scales between spaceti... | 12.831912 | 12.872421 | 13.741569 | 12.375069 | 11.989594 | 13.138067 | 11.655611 | 12.591727 | 12.04882 | 14.091096 | 11.846145 | 12.409614 | 13.114323 | 11.900305 | 12.214778 | 12.465068 | 11.882862 | 11.955032 | 12.406925 | 13.197908 | 12.005417 |
1706.04587 | Matheus Ara\'ujo Marques | L. Losano, M.A. Marques and R. Menezes | Generalized scalar field models with the same energy density and linear
stability | 6 pages, 4 figures | Phys. Lett. B 775 (2017) 178 | 10.1016/j.physletb.2017.10.064 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study how the properties of a Lagrangian density for a single real scalar
field in flat spacetime change with inclusion of an overall factor depending
only on the field. The focus of the paper is to obtain analytical results. So,
we show that even though it is possible to perform a field redefinition to get
an equ... | [
{
"created": "Wed, 14 Jun 2017 17:01:05 GMT",
"version": "v1"
}
] | 2017-11-20 | [
[
"Losano",
"L.",
""
],
[
"Marques",
"M. A.",
""
],
[
"Menezes",
"R.",
""
]
] | We study how the properties of a Lagrangian density for a single real scalar field in flat spacetime change with inclusion of an overall factor depending only on the field. The focus of the paper is to obtain analytical results. So, we show that even though it is possible to perform a field redefinition to get an equiv... | 9.663126 | 8.393566 | 9.264595 | 9.093534 | 8.829618 | 8.649347 | 8.844829 | 9.09323 | 8.24481 | 9.525553 | 8.335832 | 8.876676 | 9.478032 | 9.287354 | 9.240421 | 9.079391 | 9.182257 | 9.073367 | 9.225807 | 9.141333 | 8.935389 |
2103.03267 | David Osten | David Osten | Currents, charges and algebras in exceptional generalised geometry | 24+9 pages, version 2: comparison to the M5-brane current of Hatsuda
and Kamimura added, references added | null | 10.1007/JHEP06(2021)070 | null | hep-th math-ph math.MP | http://creativecommons.org/licenses/by/4.0/ | A classical $E_{d(d)}$-invariant Hamiltonian formulation of world-volume
theories of half-BPS p-branes in type IIb and eleven-dimensional supergravity
is proposed, extending known results to $d \leq 6$. It consists of a
Hamiltonian, characterised by a generalised metric, and a current algebra
constructed s.t. it repr... | [
{
"created": "Thu, 4 Mar 2021 19:01:54 GMT",
"version": "v1"
},
{
"created": "Mon, 22 Mar 2021 12:17:55 GMT",
"version": "v2"
}
] | 2021-06-30 | [
[
"Osten",
"David",
""
]
] | A classical $E_{d(d)}$-invariant Hamiltonian formulation of world-volume theories of half-BPS p-branes in type IIb and eleven-dimensional supergravity is proposed, extending known results to $d \leq 6$. It consists of a Hamiltonian, characterised by a generalised metric, and a current algebra constructed s.t. it reprod... | 9.334905 | 9.370967 | 11.159685 | 9.00726 | 9.523305 | 9.663587 | 9.467338 | 9.053705 | 8.74703 | 11.733891 | 8.927684 | 8.67702 | 9.590508 | 8.625566 | 8.563119 | 8.69756 | 9.008918 | 8.600266 | 8.726738 | 9.627884 | 8.632779 |
2311.16968 | Andjelo Samsarov | Nikola Herceg, Tajron Juri\'c, Andjelo Samsarov, Ivica Smoli\'c | Towards gravitational QNM spectrum from quantum spacetime | 9 pages, 1 figure; presented and prepared for "the XII. International
Symposium on Quantum Theory and Symmetries" (QTS12) and "XXVII. International
Conference on Integrable Systems and Quantum Symmetries" (ISQS27),July 24-28
2023., Prague | null | null | RBI-ThPhys-2023-46 | hep-th | http://creativecommons.org/licenses/by/4.0/ | The effective potential for the axial mode of gravitational wave on
noncommutative Schwarzschild background is presented.
Noncommutativity is introduced via deformed Hopf algebra of diffeomorphisms
by means of a semi-Killing Drinfeld twist.
The analysis is performed up to the first order in perturbation of the me... | [
{
"created": "Tue, 28 Nov 2023 17:14:53 GMT",
"version": "v1"
}
] | 2023-11-29 | [
[
"Herceg",
"Nikola",
""
],
[
"Jurić",
"Tajron",
""
],
[
"Samsarov",
"Andjelo",
""
],
[
"Smolić",
"Ivica",
""
]
] | The effective potential for the axial mode of gravitational wave on noncommutative Schwarzschild background is presented. Noncommutativity is introduced via deformed Hopf algebra of diffeomorphisms by means of a semi-Killing Drinfeld twist. The analysis is performed up to the first order in perturbation of the metric a... | 9.684943 | 10.221445 | 9.37549 | 8.663683 | 9.367943 | 8.91143 | 10.195212 | 8.958234 | 8.888168 | 10.867322 | 8.795301 | 9.767259 | 9.016443 | 8.912243 | 9.776534 | 9.421941 | 9.346682 | 8.912616 | 9.010596 | 8.956009 | 9.062088 |
2312.11610 | Liang Ma | Peng-Ju Hu, Liang Ma, H. Lu and Yi Pang | Improved Reall-Santos method for AdS black holes in general 4-derivative
gravities | LateX; 33 pages; accepted by SCIENCE CHINA Physics, Mechanics &
Astronomy | Sci. China Phys. Mech. Astron. 67 (2024) 8, 280412 | 10.1007/s11433-024-2398-1 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For asymptotically flat black holes, Reall-Santos method is a convenient tool
to compute leading higher derivative corrections to the thermodynamic
quantities without actually solving the modified field equations. However,
there are subtleties in its generalization to asymptotically AdS black holes
with general highe... | [
{
"created": "Mon, 18 Dec 2023 19:00:00 GMT",
"version": "v1"
},
{
"created": "Mon, 5 Feb 2024 07:13:51 GMT",
"version": "v2"
},
{
"created": "Wed, 17 Apr 2024 13:50:40 GMT",
"version": "v3"
}
] | 2024-07-30 | [
[
"Hu",
"Peng-Ju",
""
],
[
"Ma",
"Liang",
""
],
[
"Lu",
"H.",
""
],
[
"Pang",
"Yi",
""
]
] | For asymptotically flat black holes, Reall-Santos method is a convenient tool to compute leading higher derivative corrections to the thermodynamic quantities without actually solving the modified field equations. However, there are subtleties in its generalization to asymptotically AdS black holes with general higher ... | 7.297152 | 7.16397 | 7.434235 | 6.938137 | 7.646878 | 7.73094 | 7.546256 | 7.193487 | 7.162504 | 7.968722 | 7.225374 | 7.123746 | 7.302203 | 7.161448 | 7.029815 | 7.005723 | 7.281692 | 7.213857 | 7.199172 | 7.547108 | 7.26638 |
1910.07607 | Victoria Martin | Cynthia Keeler, Victoria L. Martin and Andrew Svesko | BTZ one-loop determinants via the Selberg zeta function for general spin | null | null | 10.1007/JHEP10(2020)138 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We relate the heat kernel and quasinormal mode methods of computing the
1-loop partition function of arbitrary spin fields on a rotating (Euclidean)
BTZ background using the Selberg zeta function associated with
$\mathbb{H}^{3}/\mathbb{Z}$, extending (1811.08433). Previously, Perry and
Williams showed for a scalar fi... | [
{
"created": "Wed, 16 Oct 2019 20:58:22 GMT",
"version": "v1"
}
] | 2020-12-02 | [
[
"Keeler",
"Cynthia",
""
],
[
"Martin",
"Victoria L.",
""
],
[
"Svesko",
"Andrew",
""
]
] | We relate the heat kernel and quasinormal mode methods of computing the 1-loop partition function of arbitrary spin fields on a rotating (Euclidean) BTZ background using the Selberg zeta function associated with $\mathbb{H}^{3}/\mathbb{Z}$, extending (1811.08433). Previously, Perry and Williams showed for a scalar fiel... | 13.649954 | 11.396478 | 14.417183 | 11.059954 | 12.757547 | 13.157289 | 12.553227 | 11.879632 | 12.740623 | 16.447454 | 11.89257 | 12.210622 | 12.838544 | 12.341471 | 12.323656 | 12.961103 | 12.231173 | 12.672051 | 12.277905 | 13.395215 | 12.296481 |
hep-th/9810007 | Jorge Ananias Neto | Petr M. Lavrov, Jorge Ananias Neto and Wilson Oliveira | A proposal for a generalized canonical osp(1,2) quantization of
dynamical systems with constraints | Revised version. To appear in Mod.Phys.Lett.A | null | 10.1142/S0217732399000626 | DF/UFJF-98-03 | hep-th | null | The aim of this paper is to consider a possibility of constructing for
arbitrary dynamical systems with first-class constraints a generalized
canonical quantization method based on the osp(1,2) supersymmetry principle.
This proposal can be considered as a counterpart to the osp(1,2)-covariant
Lagrangian quantization ... | [
{
"created": "Thu, 1 Oct 1998 14:34:14 GMT",
"version": "v1"
},
{
"created": "Mon, 15 Mar 1999 14:22:36 GMT",
"version": "v2"
}
] | 2015-06-26 | [
[
"Lavrov",
"Petr M.",
""
],
[
"Neto",
"Jorge Ananias",
""
],
[
"Oliveira",
"Wilson",
""
]
] | The aim of this paper is to consider a possibility of constructing for arbitrary dynamical systems with first-class constraints a generalized canonical quantization method based on the osp(1,2) supersymmetry principle. This proposal can be considered as a counterpart to the osp(1,2)-covariant Lagrangian quantization me... | 7.478891 | 7.043189 | 8.072062 | 7.010484 | 7.307808 | 6.840482 | 7.163311 | 6.654955 | 5.955449 | 8.108977 | 6.578138 | 6.833448 | 7.221113 | 7.040421 | 6.976711 | 7.068072 | 7.041827 | 7.057363 | 7.078738 | 7.170479 | 6.809125 |
hep-th/0108034 | Martin Schaden | Martin Schaden | Mass Generation, Ghost Condensation and Broken Symmetry: SU(2) in
Covariant Abelian Gauges | 11 pages, Latex with 2 postscript figures, uses psfig. Talk given at
Confinement IV, Vienna 2000 | null | 10.1142/9789812778567_0026 | null | hep-th | null | The local action of an SU(2) gauge theory in general covariant Abelian gauges
and the associated equivariant BRST symmetry that guarantees the perturbative
renormalizability of the model are given. A global SL(2,R) symmetry of the
model is spontaneously broken by ghost-antighost condensation at arbitrarily
small coup... | [
{
"created": "Tue, 7 Aug 2001 01:56:23 GMT",
"version": "v1"
}
] | 2017-08-23 | [
[
"Schaden",
"Martin",
""
]
] | The local action of an SU(2) gauge theory in general covariant Abelian gauges and the associated equivariant BRST symmetry that guarantees the perturbative renormalizability of the model are given. A global SL(2,R) symmetry of the model is spontaneously broken by ghost-antighost condensation at arbitrarily small coupli... | 9.759734 | 7.498801 | 9.489175 | 7.725331 | 7.389076 | 6.51609 | 6.670834 | 6.906598 | 7.973661 | 9.683346 | 7.452067 | 8.317638 | 9.138675 | 8.493546 | 8.180885 | 8.194766 | 8.297313 | 8.206395 | 8.646949 | 9.022953 | 8.671298 |
hep-th/9912017 | Klaus Bering | K. Bering (IFT) | Family of Boundary Poisson Brackets | 6 pages, LaTeX. v2: Typo in Eq. (5.1) corrected | Phys.Lett. B486 (2000) 426-430 | 10.1016/S0370-2693(00)00778-4 | UFIFT-HEP-99-18 | hep-th | null | We find a new d-parameter family of ultra-local boundary Poisson brackets
that satisfy the Jacobi identity. The two already known cases (hep-th/9305133,
hep-th/9806249 and hep-th/9901112) of ultra-local boundary Poisson brackets are
included in this new continuous family as special cases.
| [
{
"created": "Thu, 2 Dec 1999 23:37:02 GMT",
"version": "v1"
},
{
"created": "Fri, 3 Dec 1999 23:44:47 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Bering",
"K.",
"",
"IFT"
]
] | We find a new d-parameter family of ultra-local boundary Poisson brackets that satisfy the Jacobi identity. The two already known cases (hep-th/9305133, hep-th/9806249 and hep-th/9901112) of ultra-local boundary Poisson brackets are included in this new continuous family as special cases. | 14.747441 | 12.173157 | 12.908984 | 11.599067 | 12.262552 | 12.875714 | 12.409398 | 10.755659 | 12.201211 | 15.81536 | 11.230419 | 13.234763 | 13.808475 | 12.09637 | 12.210404 | 13.270015 | 12.551776 | 12.50581 | 12.999265 | 13.071245 | 11.946032 |
0809.5236 | Kostyantyn Ropotenko | K.Ropotenko | What is the maximum rate at which entropy of a string can increase? | 11 pages, no figures; formulas (18), (20) are corrected (the quantum
constant is added), a point concerning a relation between the Hawking and
Hagedorn temperatures is corrected, conclusions unchanged; accepted by
Physical Review D for publication | Phys.Rev.D79:064003,2009 | 10.1103/PhysRevD.79.064003 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | According to Susskind, a string falling toward a black hole spreads
exponentially over the stretched horizon due to repulsive interactions of the
string bits. In this paper such a string is modeled as a self-avoiding walk and
the string entropy is found. It is shown that the rate at which
information/entropy containe... | [
{
"created": "Tue, 30 Sep 2008 15:55:54 GMT",
"version": "v1"
},
{
"created": "Thu, 15 Jan 2009 08:20:33 GMT",
"version": "v2"
},
{
"created": "Thu, 26 Feb 2009 07:32:39 GMT",
"version": "v3"
}
] | 2009-12-01 | [
[
"Ropotenko",
"K.",
""
]
] | According to Susskind, a string falling toward a black hole spreads exponentially over the stretched horizon due to repulsive interactions of the string bits. In this paper such a string is modeled as a self-avoiding walk and the string entropy is found. It is shown that the rate at which information/entropy contained ... | 10.215303 | 9.808323 | 8.796413 | 8.284488 | 9.759598 | 8.550429 | 8.639155 | 8.066263 | 8.703903 | 10.036329 | 8.589857 | 9.026723 | 9.386355 | 8.836652 | 9.108237 | 8.442361 | 8.980262 | 8.859045 | 8.688922 | 9.256819 | 8.962312 |
1305.2797 | Byungwoo Kang | Byungwoo Kang | Bulk Cluster Decomposition in AdS/CFT and A No-Go Theorem for
Correlators in Microstates of Extremal Black Holes | 17 pages. Clarified some statements | null | null | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Applying the thermo-field double formalism to extremal black holes in AdS
with a macroscopic horizon, we show that (1) there exists a natural basis for
the degenerate microstates of an extremal black hole, and (2) cluster
decomposition in the bulk implies that all correlators are exactly the same for
every microstate... | [
{
"created": "Mon, 13 May 2013 14:52:00 GMT",
"version": "v1"
},
{
"created": "Sun, 19 May 2013 07:36:35 GMT",
"version": "v2"
}
] | 2013-05-21 | [
[
"Kang",
"Byungwoo",
""
]
] | Applying the thermo-field double formalism to extremal black holes in AdS with a macroscopic horizon, we show that (1) there exists a natural basis for the degenerate microstates of an extremal black hole, and (2) cluster decomposition in the bulk implies that all correlators are exactly the same for every microstate o... | 7.665 | 8.573049 | 9.558835 | 8.010723 | 8.290768 | 8.365056 | 8.454972 | 8.430003 | 7.825157 | 10.075123 | 7.618054 | 7.687874 | 7.828125 | 7.415073 | 7.600208 | 7.477383 | 7.782997 | 7.665939 | 7.319924 | 7.788276 | 7.420743 |
hep-th/9408010 | J. Baacke | J. Baacke and T. Daiber (Dortmund University) | One-loop corrections to the instanton transition in the two-dimensional
Abelian Higgs model | DO-TH-94/17, 20 pages, 4 figures appended as uucompressed .eps files,
LaTeX, needs epsfig.sty | Phys.Rev. D51 (1995) 795-801 | 10.1103/PhysRevD.51.795 | null | hep-th hep-lat hep-ph | null | We present an evaluation of the fluctuation determinant which appears as a
prefactor in the instanton transition rate for the two-dimensional Abelian
Higgs model. The corrections are found to change the rate at most by a factor
of 2 for 0.4 < M_W/M_H < 2.0.
| [
{
"created": "Tue, 2 Aug 1994 14:07:04 GMT",
"version": "v1"
}
] | 2009-10-28 | [
[
"Baacke",
"J.",
"",
"Dortmund University"
],
[
"Daiber",
"T.",
"",
"Dortmund University"
]
] | We present an evaluation of the fluctuation determinant which appears as a prefactor in the instanton transition rate for the two-dimensional Abelian Higgs model. The corrections are found to change the rate at most by a factor of 2 for 0.4 < M_W/M_H < 2.0. | 10.939363 | 9.350388 | 9.116271 | 8.3345 | 8.656401 | 10.034404 | 9.570428 | 9.531092 | 8.706594 | 9.113396 | 9.71517 | 8.982954 | 9.456289 | 9.096793 | 9.732657 | 9.61344 | 9.523214 | 9.777983 | 9.160432 | 10.548028 | 9.646384 |
hep-th/9711199 | Javier Borlaf | E. Alvarez, J. Borlaf and J.H. Le\'on | Killings, Duality and Characteristic Polynomials | 14 pages, Latex | Phys.Lett. B421 (1998) 162-168 | 10.1016/S0370-2693(97)01585-2 | IFT-UAM/CSIC-97-01 | hep-th | null | In this paper the complete geometrical setting of (lowest order) abelian
T-duality is explored with the help of some new geometrical tools (the reduced
formalism). In particular, all invariant polynomials (the integrands of the
characteristic classes) can be explicitly computed for the dual model in terms
of quantiti... | [
{
"created": "Thu, 27 Nov 1997 13:19:33 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Alvarez",
"E.",
""
],
[
"Borlaf",
"J.",
""
],
[
"León",
"J. H.",
""
]
] | In this paper the complete geometrical setting of (lowest order) abelian T-duality is explored with the help of some new geometrical tools (the reduced formalism). In particular, all invariant polynomials (the integrands of the characteristic classes) can be explicitly computed for the dual model in terms of quantities... | 20.12068 | 19.071138 | 20.078844 | 18.217203 | 21.413731 | 23.196259 | 20.30286 | 17.03207 | 18.729025 | 22.822472 | 18.513557 | 17.998541 | 18.410093 | 17.279543 | 17.767929 | 17.383329 | 17.537901 | 17.234846 | 16.683851 | 18.084793 | 16.980658 |
hep-th/9605095 | null | Matthias Blau, Ian Jermyn, George Thompson | Solving Topological Field Theories on Mapping Tori | 16 pages, LaTeX file | Phys.Lett. B383 (1996) 169-178 | 10.1016/0370-2693(96)00728-9 | IC/96/74, ENSLAPP-L-590/96 | hep-th | null | Using gauge theory and functional integral methods, we derive concrete
expressions for the partition functions of BF theory and the U(1|1) model of
Rozansky and Saleur on $\Sigma x S^{1}$, both directly and using equivalent
two-dimensional theories. We also derive the partition function of a certain
non-abelian gener... | [
{
"created": "Tue, 14 May 1996 13:42:26 GMT",
"version": "v1"
}
] | 2009-10-30 | [
[
"Blau",
"Matthias",
""
],
[
"Jermyn",
"Ian",
""
],
[
"Thompson",
"George",
""
]
] | Using gauge theory and functional integral methods, we derive concrete expressions for the partition functions of BF theory and the U(1|1) model of Rozansky and Saleur on $\Sigma x S^{1}$, both directly and using equivalent two-dimensional theories. We also derive the partition function of a certain non-abelian general... | 8.314713 | 8.715154 | 9.438938 | 8.666802 | 8.58367 | 9.126279 | 9.205021 | 8.709453 | 8.762619 | 10.369098 | 8.310172 | 8.203856 | 8.738955 | 7.90159 | 7.930429 | 7.977574 | 8.220273 | 8.001467 | 8.076948 | 8.242424 | 8.311216 |
1511.01108 | Julio Alberto M\'endez | Eloy Ay\'on-Beato, Daniel Higuita-Borja, Julio A. M\'endez-Zavaleta | Rotating (A)dS black holes in bigravity | 8 pages | Phys. Rev. D 93, 024049 (2016) | 10.1103/PhysRevD.93.024049 | null | hep-th gr-qc | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we explore the advantage of using the Kerr-Schild Ansatz in the
search of analytic configurations to bigravity. It turns out that it plays a
crucial role by providing means to straightforwardly calculate the square root
matrix encoding the interaction terms between both gravities. We rederive in
this sp... | [
{
"created": "Tue, 3 Nov 2015 21:06:30 GMT",
"version": "v1"
},
{
"created": "Fri, 5 Feb 2016 01:11:51 GMT",
"version": "v2"
},
{
"created": "Mon, 17 Jul 2017 07:50:30 GMT",
"version": "v3"
}
] | 2017-07-18 | [
[
"Ayón-Beato",
"Eloy",
""
],
[
"Higuita-Borja",
"Daniel",
""
],
[
"Méndez-Zavaleta",
"Julio A.",
""
]
] | In this paper we explore the advantage of using the Kerr-Schild Ansatz in the search of analytic configurations to bigravity. It turns out that it plays a crucial role by providing means to straightforwardly calculate the square root matrix encoding the interaction terms between both gravities. We rederive in this spir... | 12.262599 | 13.106537 | 12.038526 | 12.754716 | 11.796054 | 12.466347 | 12.179917 | 11.576642 | 12.639744 | 13.455375 | 11.89401 | 11.800294 | 12.202838 | 11.657275 | 11.73278 | 11.41513 | 11.85768 | 11.426953 | 11.938416 | 11.742093 | 11.81724 |
1806.09072 | Jung Hun Lee | Chanyong Park, Daeho Ro, Jung Hun Lee | c-theorem of the entanglement entropy | 24 pages, 8 figures | null | 10.1007/JHEP11(2018)165 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We holographically investigate the renormalization group flow in a
two-dimensional conformal field theory deformed by a relevant operator. If the
relevant operator allows another fixed point, the UV conformal field theory
smoothly flows to a new IR conformal field theory. From the holographic point
of view, such a re... | [
{
"created": "Sun, 24 Jun 2018 02:55:23 GMT",
"version": "v1"
}
] | 2018-12-05 | [
[
"Park",
"Chanyong",
""
],
[
"Ro",
"Daeho",
""
],
[
"Lee",
"Jung Hun",
""
]
] | We holographically investigate the renormalization group flow in a two-dimensional conformal field theory deformed by a relevant operator. If the relevant operator allows another fixed point, the UV conformal field theory smoothly flows to a new IR conformal field theory. From the holographic point of view, such a reno... | 7.62182 | 6.246267 | 7.588024 | 6.894624 | 6.489749 | 6.30724 | 6.674722 | 6.177746 | 6.607729 | 8.507289 | 6.595442 | 7.053427 | 7.261978 | 7.118488 | 7.014226 | 6.902176 | 7.187779 | 6.812812 | 7.208026 | 7.294928 | 7.033115 |
hep-th/0309172 | Ali Serdar Arikan | Abdullah Algin, Metin Arik, Ali Serdar Arikan | Two-parameter deformed supersymmetric oscillators with
SUq1/q2(n|m)-covariance | 10 pages | Mod.Phys.Lett.A20:613-622,2005 | 10.1142/S0217732305015781 | null | hep-th | null | A two-parameter deformed superoscillator system with SUq1/q2(n|m)-covariance
is presented and used to construct a two-parameter deformed N=2 SUSY algebra.
The Fock space representation of the algebra is discussed and the deformed
Hamiltonian for such generalized superoscillators is obtained.
| [
{
"created": "Wed, 17 Sep 2003 07:38:15 GMT",
"version": "v1"
},
{
"created": "Thu, 25 Mar 2004 12:14:37 GMT",
"version": "v2"
}
] | 2011-07-28 | [
[
"Algin",
"Abdullah",
""
],
[
"Arik",
"Metin",
""
],
[
"Arikan",
"Ali Serdar",
""
]
] | A two-parameter deformed superoscillator system with SUq1/q2(n|m)-covariance is presented and used to construct a two-parameter deformed N=2 SUSY algebra. The Fock space representation of the algebra is discussed and the deformed Hamiltonian for such generalized superoscillators is obtained. | 13.527155 | 11.632846 | 15.655041 | 11.233644 | 12.108936 | 14.221252 | 13.208248 | 12.913005 | 10.576872 | 14.782778 | 11.887788 | 11.482171 | 14.869976 | 11.782634 | 11.203293 | 12.420083 | 11.71381 | 12.210398 | 10.812347 | 13.404124 | 11.121135 |
2305.02895 | Lin Yi-Yu | Yi-Yu Lin | Distilled density matrices of holographic PEE from thread-state
correspondence | 34 pages,7 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | Within the framework of holographic duality, CMI (conditional mutual
information) is often understood as a correlation between ``region pairs" and
is closely related to the concept of partial entanglement entropy (PEE). The
main theme of this paper is to try to understand the rigorous physical meaning
of such a regio... | [
{
"created": "Thu, 4 May 2023 15:03:26 GMT",
"version": "v1"
}
] | 2023-05-05 | [
[
"Lin",
"Yi-Yu",
""
]
] | Within the framework of holographic duality, CMI (conditional mutual information) is often understood as a correlation between ``region pairs" and is closely related to the concept of partial entanglement entropy (PEE). The main theme of this paper is to try to understand the rigorous physical meaning of such a region-... | 17.189703 | 16.535664 | 18.185438 | 16.349373 | 16.841473 | 15.89265 | 15.464612 | 15.75188 | 16.433048 | 20.213188 | 14.000319 | 15.971998 | 16.087814 | 15.975727 | 16.573698 | 15.792321 | 15.971084 | 15.549209 | 16.21759 | 17.221132 | 15.231125 |
hep-th/9607237 | Raimar Wulkenhaar | Raimar Wulkenhaar | Grand Unification in Non-Associative Geometry | 48 pages, LaTeX2e + AMS macros + graphics.sty + eps table; revised
version: A Majorana mass for the right neutrinos has been introduced. This
leads to an additional 50-plet of Higgs fields, and an unobserved neutral
gauge field gets a very large mass | null | null | null | hep-th | null | We formulate the flipped SU(5) x U(1)-GUT within the framework of
non-associative geometry. It suffices to take the matrix Lie algebra su(5) as
the input; the u(1)-part with its representation on the fermions is an
algebraic consequence. The occurring Higgs multiplets
(24,5,45,50-representations of su(5)) are uniquel... | [
{
"created": "Wed, 31 Jul 1996 12:54:43 GMT",
"version": "v1"
},
{
"created": "Mon, 10 Feb 1997 20:45:13 GMT",
"version": "v2"
}
] | 2008-02-03 | [
[
"Wulkenhaar",
"Raimar",
""
]
] | We formulate the flipped SU(5) x U(1)-GUT within the framework of non-associative geometry. It suffices to take the matrix Lie algebra su(5) as the input; the u(1)-part with its representation on the fermions is an algebraic consequence. The occurring Higgs multiplets (24,5,45,50-representations of su(5)) are uniquely ... | 10.202861 | 11.201886 | 10.065893 | 9.504519 | 11.037794 | 11.193602 | 10.175627 | 10.649466 | 9.809835 | 10.849151 | 9.929708 | 9.926423 | 9.733289 | 9.250553 | 9.89271 | 9.795853 | 9.66185 | 9.626066 | 9.634807 | 9.954616 | 9.36305 |
hep-th/0505099 | Radu Roiban | A. Dymarsky, I.R. Klebanov, R. Roiban | Perturbative Search for Fixed Lines in Large N Gauge Theories | 31 pages, 4 figures, latex v2: Clarifications and reference added | JHEP 0508 (2005) 011 | 10.1088/1126-6708/2005/08/011 | null | hep-th hep-ph | null | The logarithmic running of marginal double-trace operators is a general
feature of 4-d field theories containing scalar fields in the adjoint or
bifundamental representation. Such operators provide leading contributions in
the large N limit; therefore, the leading terms in their beta functions must
vanish for a theor... | [
{
"created": "Wed, 11 May 2005 19:39:03 GMT",
"version": "v1"
},
{
"created": "Tue, 7 Jun 2005 13:24:35 GMT",
"version": "v2"
}
] | 2009-11-11 | [
[
"Dymarsky",
"A.",
""
],
[
"Klebanov",
"I. R.",
""
],
[
"Roiban",
"R.",
""
]
] | The logarithmic running of marginal double-trace operators is a general feature of 4-d field theories containing scalar fields in the adjoint or bifundamental representation. Such operators provide leading contributions in the large N limit; therefore, the leading terms in their beta functions must vanish for a theory ... | 6.898384 | 6.238597 | 7.657694 | 6.735837 | 7.202501 | 6.890224 | 7.093993 | 7.10503 | 6.683186 | 8.475193 | 6.752424 | 6.621974 | 6.872637 | 6.643142 | 6.676944 | 6.810657 | 6.752733 | 6.935181 | 6.701088 | 7.065834 | 6.791263 |
1311.1512 | Martin Sprenger | J. Bartels, J. Kotanski, V. Schomerus, M. Sprenger | The Excited Hexagon Reloaded | 6 pages | null | null | DESY 13-197 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work revisits the computation of six-gluon scattering amplitudes in the
high energy limit of strongly coupled N=4 supersymmetric Yang-Mills theory. It
is based on previous studies in which we showed that the amplitude simplifies
in the Regge regime and outlined an efficient computational scheme. By
exploiting a ... | [
{
"created": "Wed, 6 Nov 2013 21:00:03 GMT",
"version": "v1"
}
] | 2013-11-08 | [
[
"Bartels",
"J.",
""
],
[
"Kotanski",
"J.",
""
],
[
"Schomerus",
"V.",
""
],
[
"Sprenger",
"M.",
""
]
] | This work revisits the computation of six-gluon scattering amplitudes in the high energy limit of strongly coupled N=4 supersymmetric Yang-Mills theory. It is based on previous studies in which we showed that the amplitude simplifies in the Regge regime and outlined an efficient computational scheme. By exploiting a sy... | 8.613242 | 8.570067 | 8.221296 | 7.85868 | 8.203691 | 8.109428 | 8.329939 | 7.759414 | 8.077629 | 8.892323 | 8.231413 | 8.265935 | 8.393486 | 8.212124 | 8.379142 | 8.448331 | 8.148512 | 8.143747 | 8.041613 | 8.251667 | 8.182897 |
hep-th/0208090 | Osman Teoman Turgut | O. Teoman Turgut (Bogazici University, Istanbul, and KTH, Stockholm,
and Feza Gursey Institute, Istanbul) | On two dimensional coupled bosons and fermions | 25 pages, no figures | J.Math.Phys. 44 (2003) 198-219 | 10.1063/1.1516846 | null | hep-th | null | We study complex bosons and fermions coupled through a generalized Yukawa
type coupling in the large-N_c limit following ideas of Rajeev [Int. Jour. Mod.
Phys. A 9 (1994) 5583]. We study a linear approximation to this model. We show
that in this approximation we do not have boson-antiboson and
fermion-antifermion bou... | [
{
"created": "Tue, 13 Aug 2002 14:07:18 GMT",
"version": "v1"
}
] | 2009-11-07 | [
[
"Turgut",
"O. Teoman",
"",
"Bogazici University, Istanbul, and KTH, Stockholm,\n and Feza Gursey Institute, Istanbul"
]
] | We study complex bosons and fermions coupled through a generalized Yukawa type coupling in the large-N_c limit following ideas of Rajeev [Int. Jour. Mod. Phys. A 9 (1994) 5583]. We study a linear approximation to this model. We show that in this approximation we do not have boson-antiboson and fermion-antifermion bound... | 8.648943 | 9.966962 | 9.636399 | 8.982326 | 9.727184 | 9.242548 | 9.882668 | 8.705029 | 8.742586 | 9.428341 | 8.622625 | 8.606463 | 9.031131 | 8.615785 | 8.417119 | 8.491975 | 8.955244 | 8.668846 | 8.655738 | 9.06098 | 8.334671 |
1506.04589 | Leonardo Modesto | Pietro Don\`a, Stefano Giaccari, Leonardo Modesto, Leslaw Rachwal,
Yiwei Zhu | Scattering amplitudes in super-renormalizable gravity | 25 pages, 2 Figures | null | 10.1007/JHEP08(2015)038 | null | hep-th gr-qc hep-ph math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We explicitly compute the tree-level on-shell four-graviton amplitudes in
four, five and six dimensions for local and weakly nonlocal gravitational
theories that are quadratic in both, the Ricci and scalar curvature with form
factors of the d'Alembertian operator inserted between. More specifically we
are interested ... | [
{
"created": "Mon, 15 Jun 2015 13:21:07 GMT",
"version": "v1"
}
] | 2015-09-30 | [
[
"Donà",
"Pietro",
""
],
[
"Giaccari",
"Stefano",
""
],
[
"Modesto",
"Leonardo",
""
],
[
"Rachwal",
"Leslaw",
""
],
[
"Zhu",
"Yiwei",
""
]
] | We explicitly compute the tree-level on-shell four-graviton amplitudes in four, five and six dimensions for local and weakly nonlocal gravitational theories that are quadratic in both, the Ricci and scalar curvature with form factors of the d'Alembertian operator inserted between. More specifically we are interested in... | 6.945434 | 7.232423 | 7.993419 | 7.279528 | 7.360628 | 7.549791 | 7.429798 | 7.562314 | 7.356798 | 8.134392 | 7.011766 | 7.028157 | 7.24849 | 7.005906 | 6.930839 | 7.043845 | 7.037542 | 7.132261 | 6.836775 | 7.27835 | 6.993331 |
hep-th/0104216 | Peter Jarvis | H S Booth, G Legg and P D Jarvis | Algebraic solution for the vector potential in the Dirac equation | 14 pages, LaTeX | J.Phys.A34:5667-5678,2001 | 10.1088/0305-4470/34/28/304 | University of Tasmania UTAS-PHYS-01-02 | hep-th math-ph math.MP | null | The Dirac equation for an electron in an external electromagnetic field can
be regarded as a singular set of linear equations for the vector potential.
Radford's method of algebraically solving for the vector potential is reviewed,
with attention to the additional constraints arising from non-maximality of the
rank. ... | [
{
"created": "Wed, 25 Apr 2001 01:38:13 GMT",
"version": "v1"
}
] | 2008-11-26 | [
[
"Booth",
"H S",
""
],
[
"Legg",
"G",
""
],
[
"Jarvis",
"P D",
""
]
] | The Dirac equation for an electron in an external electromagnetic field can be regarded as a singular set of linear equations for the vector potential. Radford's method of algebraically solving for the vector potential is reviewed, with attention to the additional constraints arising from non-maximality of the rank. Th... | 14.041757 | 16.182198 | 16.455158 | 12.845025 | 13.934612 | 15.013444 | 13.697692 | 13.455525 | 12.465933 | 15.637411 | 13.383445 | 13.282932 | 12.948195 | 12.786182 | 12.906301 | 12.585368 | 12.888684 | 12.589665 | 12.708271 | 13.68734 | 12.554613 |
0904.4509 | Michael Ambroso | Michael Ambroso and Burt Ovrut | The B-L/Electroweak Hierarchy in Heterotic String and M-Theory | 16 pages; typos fixed, analysis generalized | JHEP 0910:011, 2009 | 10.1088/1126-6708/2009/10/011 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | E8 x E8 heterotic string and M-theory, when compactified on a Calabi-Yau
threefold admitting an SU(4) vector bundle with Wilson lines, can give rise to
the exact MSSM spectrum with three right-handed neutrino chiral superields, one
per family. Rank preserving Wilson lines require that the standard model group
be augm... | [
{
"created": "Wed, 29 Apr 2009 19:19:47 GMT",
"version": "v1"
},
{
"created": "Wed, 10 Jun 2009 22:59:53 GMT",
"version": "v2"
},
{
"created": "Tue, 6 Oct 2009 23:20:28 GMT",
"version": "v3"
}
] | 2009-10-12 | [
[
"Ambroso",
"Michael",
""
],
[
"Ovrut",
"Burt",
""
]
] | E8 x E8 heterotic string and M-theory, when compactified on a Calabi-Yau threefold admitting an SU(4) vector bundle with Wilson lines, can give rise to the exact MSSM spectrum with three right-handed neutrino chiral superields, one per family. Rank preserving Wilson lines require that the standard model group be augmen... | 9.323483 | 8.767475 | 8.90123 | 8.078339 | 7.697752 | 8.061634 | 7.876813 | 7.535985 | 8.442328 | 9.249746 | 8.313834 | 8.343375 | 8.856134 | 8.527232 | 8.445938 | 8.330836 | 8.174951 | 8.400208 | 8.584946 | 8.935237 | 8.508374 |
hep-th/0303210 | Tsunehide Kuroki | Hikaru Kawai, Tsunehide Kuroki and Takeshi Morita | Dijkgraaf-Vafa theory as large-N reduction | 34 pages, LaTeX, to appear in Nucl. Phys. B | Nucl.Phys. B664 (2003) 185-212 | 10.1016/S0550-3213(03)00408-5 | null | hep-th | null | We construct a large-N twisted reduced model of the four-dimensional super
Yang-Mills theory coupled to one adjoint matter. We first consider a
non-commutative version of the four-dimensional superspace, and then give the
mapping rule between matrices and functions on this space explicitly. The
supersymmetry is reali... | [
{
"created": "Mon, 24 Mar 2003 20:21:08 GMT",
"version": "v1"
},
{
"created": "Fri, 4 Apr 2003 14:47:35 GMT",
"version": "v2"
},
{
"created": "Thu, 29 May 2003 16:12:36 GMT",
"version": "v3"
}
] | 2010-04-05 | [
[
"Kawai",
"Hikaru",
""
],
[
"Kuroki",
"Tsunehide",
""
],
[
"Morita",
"Takeshi",
""
]
] | We construct a large-N twisted reduced model of the four-dimensional super Yang-Mills theory coupled to one adjoint matter. We first consider a non-commutative version of the four-dimensional superspace, and then give the mapping rule between matrices and functions on this space explicitly. The supersymmetry is realize... | 9.047799 | 8.285402 | 9.556524 | 8.027039 | 8.633703 | 8.357274 | 8.228654 | 8.746466 | 8.429693 | 10.346585 | 8.116833 | 8.510216 | 8.816427 | 8.308085 | 8.52993 | 8.32873 | 8.308151 | 8.170565 | 8.505237 | 9.0477 | 8.325073 |
1905.10555 | Kenichi Konishi | Stefano Bolognesi, Sven Bjarke Gudnason, Kenichi Konishi, Keisuke
Ohashi | Large-$N$ $\mathbb{CP}^{N-1}$ sigma model on a Euclidean torus:
uniqueness and stability of the vacuum | 40 pages, 4 figures | JHEP 1912:044, 2019 | 10.1007/JHEP12(2019)044 | IFUP-TH-2019 | hep-th hep-lat | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we examine analytically the large-$N$ gap equation and its
solution for the $2D$ $\mathbb{CP}^{N-1}$ sigma model defined on a Euclidean
spacetime torus of arbitrary shape and size ($L, \beta)$, $\beta$ being the
inverse temperature. We find that the system has a unique homogeneous phase,
with the $\math... | [
{
"created": "Sat, 25 May 2019 08:23:41 GMT",
"version": "v1"
},
{
"created": "Mon, 17 Jun 2019 16:38:10 GMT",
"version": "v2"
},
{
"created": "Fri, 22 Nov 2019 12:11:49 GMT",
"version": "v3"
}
] | 2019-12-17 | [
[
"Bolognesi",
"Stefano",
""
],
[
"Gudnason",
"Sven Bjarke",
""
],
[
"Konishi",
"Kenichi",
""
],
[
"Ohashi",
"Keisuke",
""
]
] | In this paper we examine analytically the large-$N$ gap equation and its solution for the $2D$ $\mathbb{CP}^{N-1}$ sigma model defined on a Euclidean spacetime torus of arbitrary shape and size ($L, \beta)$, $\beta$ being the inverse temperature. We find that the system has a unique homogeneous phase, with the $\mathbb... | 7.467655 | 7.806193 | 8.078671 | 7.19207 | 7.557927 | 7.57017 | 7.454387 | 7.45174 | 7.247759 | 8.221888 | 7.365547 | 6.965563 | 7.63821 | 7.300373 | 7.41355 | 7.121651 | 7.111712 | 7.1295 | 7.184631 | 7.451264 | 7.105847 |
2009.12530 | Fabio Scardigli | Luca Buoninfante, Giuseppe Gaetano Luciano, Luciano Petruzziello,
Fabio Scardigli | Bekenstein bound and uncertainty relations | 7 pages, 1 figure, version published on Phys.Lett.B (derivation
improved) | Phys.Lett.B 824 (2022) 136818 | 10.1016/j.physletb.2021.136818 | null | hep-th gr-qc quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The non zero value of Planck constant $h$ underlies the emergence of several
inequalities that must be satisfied in the quantum realm, the most prominent
one being Heisenberg Uncertainty Principle. Among these inequalities,
Bekenstein bound provides a universal limit on the entropy that can be
contained in a localize... | [
{
"created": "Sat, 26 Sep 2020 08:11:05 GMT",
"version": "v1"
},
{
"created": "Thu, 9 Dec 2021 11:01:27 GMT",
"version": "v2"
}
] | 2021-12-10 | [
[
"Buoninfante",
"Luca",
""
],
[
"Luciano",
"Giuseppe Gaetano",
""
],
[
"Petruzziello",
"Luciano",
""
],
[
"Scardigli",
"Fabio",
""
]
] | The non zero value of Planck constant $h$ underlies the emergence of several inequalities that must be satisfied in the quantum realm, the most prominent one being Heisenberg Uncertainty Principle. Among these inequalities, Bekenstein bound provides a universal limit on the entropy that can be contained in a localized ... | 8.498724 | 8.516807 | 8.729757 | 8.083546 | 8.476125 | 8.112084 | 8.356762 | 7.884808 | 8.435166 | 8.488936 | 7.605357 | 8.118087 | 7.765448 | 7.623457 | 7.846853 | 7.708368 | 7.941456 | 7.805277 | 7.690351 | 7.836306 | 7.625573 |
hep-th/9807066 | Tomohiko Takahashi | Tsuguhiko Asakawa, Taichiro Kugo and Tomohiko Takahashi | BRS Invariance of Unoriented Open-Closed String Field Theory | 53 pages, LaTeX with PTPTeX.sty, 23 eps figures, style file replaced | Prog.Theor.Phys. 100 (1998) 831-879 | 10.1143/PTP.100.831 | KUNS-1508 HE(TH) 98/06, UT-814 | hep-th | null | We present the full action for the unoriented open-closed string field theory
which is based on the \alpha=p^+ HIKKO type vertices. The BRS invariance of the
action is proved up to the terms which are expected to cancel the anomalous
one-loop contributions. This implies that the system is invariant under the
gauge tr... | [
{
"created": "Thu, 9 Jul 1998 14:01:35 GMT",
"version": "v1"
},
{
"created": "Sat, 11 Jul 1998 09:55:16 GMT",
"version": "v2"
}
] | 2009-10-31 | [
[
"Asakawa",
"Tsuguhiko",
""
],
[
"Kugo",
"Taichiro",
""
],
[
"Takahashi",
"Tomohiko",
""
]
] | We present the full action for the unoriented open-closed string field theory which is based on the \alpha=p^+ HIKKO type vertices. The BRS invariance of the action is proved up to the terms which are expected to cancel the anomalous one-loop contributions. This implies that the system is invariant under the gauge tran... | 13.935858 | 12.281498 | 15.052392 | 11.398524 | 13.722698 | 12.92728 | 12.509588 | 11.472837 | 12.024783 | 16.590216 | 11.688565 | 12.596252 | 13.081183 | 12.432062 | 12.482254 | 11.996533 | 12.196514 | 12.4309 | 13.659847 | 13.259515 | 12.339944 |
hep-th/9312119 | Pavel Etingof | Alexander Varchenko | Critical Points of the Product of Powers of Linear Functions and
Families of Bases of Singular Vectors | 15 pages, no figures, posted by Pavel Etingof by the author's request | null | null | null | hep-th math.QA | null | The quasiclassical asymptotics of the Knizhnik-Zamolodchikov equation with
values in the tensor product of sl(2)- representations are considered. The
first term of asymptotics is an eigenvector of a system of commuting operators.
We show that the norm of this vector with respect to the Shapovalov form is
equal to the... | [
{
"created": "Tue, 14 Dec 1993 16:24:25 GMT",
"version": "v1"
}
] | 2008-02-03 | [
[
"Varchenko",
"Alexander",
""
]
] | The quasiclassical asymptotics of the Knizhnik-Zamolodchikov equation with values in the tensor product of sl(2)- representations are considered. The first term of asymptotics is an eigenvector of a system of commuting operators. We show that the norm of this vector with respect to the Shapovalov form is equal to the d... | 6.005036 | 6.251467 | 7.261683 | 5.663495 | 6.592306 | 5.978705 | 6.260839 | 5.68333 | 6.203866 | 7.60848 | 5.893672 | 5.652643 | 5.996099 | 5.658442 | 5.746346 | 5.769824 | 5.810213 | 5.494565 | 5.65386 | 6.172775 | 5.698742 |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.